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Supporting files include aerial reference images for six distinct data collection \u201cRuns\u201d (I90_94_Stationary_Run_X_ref_image.png, where X equals 1, 2, 3, 4, 5, and 6). Associated centerline files are also provided for each \u201cRun\u201d (I-90-stationary-Run_X-geometry-with-ramps.csv). In each centerline file, x and y coordinates (in meters) marking each lane centerline are provided. The origin point of the reference image is located at the top left corner. Additionally, in each centerline file, an indicator variable is used for each lane to define the following types of road sections: 0=no ramp, 1=on-ramps, 2=off-ramps, and 3=weaving segments. The number attached to each column header is the numerical ID assigned for the specific lane (see \u201cTGSIM \u2013 Centerline Data Dictionary \u2013 I90_94Stationary.csv\u201d for more details). The dataset defines six northbound lanes using these centerline files. Twelve different numerical IDs are used to define the six northbound lanes (1, 2, 3, 4, 5, 6, 10, 11, 12, 13, 14, and 15) depending on the run. Images that map the lanes of interest to the numerical lane IDs referenced in the trajectory dataset are stored in the folder titled \u201cAnnotation on Regions.zip\u201d. Lane IDs are provided in the reference images in red text for each data collection run (I90_94_Stationary_Run_X_ref_image_annotated.jpg, where X equals 1, 2, 3, 4, 5, and 6). \n\nThis dataset was collected as part of the Third Generation Simulation Data (TGSIM): A Closer Look at the Impacts of Automated Driving Systems on Human Behavior project. During the project, six trajectory datasets capable of characterizing human-automated vehicle interactions under a diverse set of scenarios in highway and city environments were collected and processed. For more information, see the project report found here: https://rosap.ntl.bts.gov/view/dot/74647. This dataset, which is one of the six collected as part of the TGSIM project, contains data collected using the fixed location aerial videography approach with one high-resolution 8K camera mounted on a helicopter hovering over a short segment of I-94 focusing on the merge and diverge points in Chicago, IL. The altitude of the helicopter (approximately 213 meters) enabled the camera to capture 1.3 km of highway driving and a major weaving section in each direction (where I-90 and I-94 diverge in the northbound direction and merge in the southbound direction). The segment has two off-ramps and two on-ramps in the northbound direction. All roads have 88 kph (55 mph) speed limits. The camera captured footage during the evening rush hour (4:00 PM-6:00 PM CT) on a cloudy day. During this period, two SAE Level 2 ADAS-equipped vehicles drove through the segment, entering the northbound direction upstream of the target section, exiting the target section on the right through I-94, and attempting to perform a total of three lane-changing maneuvers (if safe to do so). These vehicles are indicated in the dataset.\n\nAs part of this dataset, the following files were provided:\n<ul><li>I90_94_stationary_final.csv contains the numerical data to be used for analysis that includes vehicle level trajectory data at every 0.1 second. Vehicle type, width, and length are provided with instantaneous location, speed, and acceleration data. All distance measurements (width, length, location) were converted from pixels to meters using the following conversion factor: 1 pixel = 0.3-meter conversion.</li>\n<li>I90_94_Stationary_Run_X_ref_image.png are the aerial reference images that define the geographic region for each run X.</li>\n<li>I-90-stationary-Run_X-geometry-with-ramps.csv contain the coordinates that define the lane centerlines for each Run X. 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Twelve different numerical IDs are used to define the six northbound lanes (1, 2, 3, 4, 5, 6, 10, 11, 12, 13, 14, and 15) depending on the run. Images that map the lanes of interest to the numerical lane IDs referenced in the trajectory dataset are stored in the folder titled \u201cAnnotation on Regions.zip\u201d. Lane IDs are provided in the reference images in red text for each data collection run (I90_94_Stationary_Run_X_ref_image_annotated.jpg, where X equals 1, 2, 3, 4, 5, and 6). \n\nThis dataset was collected as part of the Third Generation Simulation Data (TGSIM): A Closer Look at the Impacts of Automated Driving Systems on Human Behavior project. During the project, six trajectory datasets capable of characterizing human-automated vehicle interactions under a diverse set of scenarios in highway and city environments were collected and processed. For more information, see the project report found here: https://rosap.ntl.bts.gov/view/dot/74647. This dataset, which is one of the six collected as part of the TGSIM project, contains data collected using the fixed location aerial videography approach with one high-resolution 8K camera mounted on a helicopter hovering over a short segment of I-94 focusing on the merge and diverge points in Chicago, IL. The altitude of the helicopter (approximately 213 meters) enabled the camera to capture 1.3 km of highway driving and a major weaving section in each direction (where I-90 and I-94 diverge in the northbound direction and merge in the southbound direction). The segment has two off-ramps and two on-ramps in the northbound direction. All roads have 88 kph (55 mph) speed limits. The camera captured footage during the evening rush hour (4:00 PM-6:00 PM CT) on a cloudy day. During this period, two SAE Level 2 ADAS-equipped vehicles drove through the segment, entering the northbound direction upstream of the target section, exiting the target section on the right through I-94, and attempting to perform a total of three lane-changing maneuvers (if safe to do so). These vehicles are indicated in the dataset.\n\nAs part of this dataset, the following files were provided:\n<ul><li>I90_94_stationary_final.csv contains the numerical data to be used for analysis that includes vehicle level trajectory data at every 0.1 second. Vehicle type, width, and length are provided with instantaneous location, speed, and acceleration data. 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232 MB file of trajectory data (I395-final.csv) that contains position, speed, and acceleration data for non-automated passenger cars, trucks, buses, and automated vehicles on an expressway within an urban environment. Supporting files include an aerial reference image (I395_ref_image.png) and a list of polygon boundaries (I395_boundaries.csv) and associated images (I395_lane-1, I395_lane-2, \u2026, I395_lane-6) stored in a folder titled \u201cAnnotation on Regions.zip\u201d to map physical roadway segments to the numerical lane IDs referenced in the trajectory dataset. In the boundary file, columns \u201cx1\u201d to \u201cx5\u201d represent the horizontal pixel values in the reference image, with \u201cx1\u201d being the leftmost boundary line and \u201cx5\u201d being the rightmost boundary line, while the column \"y\" represents corresponding vertical pixel values. The origin point of the reference image is located at the top left corner. The dataset defines five lanes with five boundaries. Lane -6 corresponds to the area to the left of \u201cx1\u201d. Lane -5 corresponds to the area between \u201cx1\u201d and \u201cx2\u201d, and so forth to the rightmost lane, which is defined by the area to the right of \u201cx5\u201d (Lane -2). Lane -1 refers to vehicles that go onto the shoulder of the merging lane (Lane -2), which are manually separated by watching the videos.\n\nThis dataset was collected as part of the Third Generation Simulation Data (TGSIM): A Closer Look at the Impacts of Automated Driving Systems on Human Behavior project. During the project, six trajectory datasets capable of characterizing human-automated vehicle interactions under a diverse set of scenarios in highway and city environments were collected and processed. For more information, see the project report found here: https://rosap.ntl.bts.gov/view/dot/74647. This dataset, which was one of the six collected as part of the TGSIM project, contains data collected from six 4K cameras mounted on tripods, positioned on three overpasses along I-395 in Washington, D.C. The cameras captured distinct segments of the highway, and their combined overlapping and non-overlapping footage resulted in a continuous trajectory for the entire section covering 0.5 km. This section covers a major weaving/mandatory lane-changing between L'Enfant Plaza and 4th Street SW, with three lanes in the eastbound direction and a major on-ramp on the left side. In addition to the on-ramp, the section covers an off-ramp on the right side. The expressway includes one diverging lane at the beginning of the section on the right side and one merging lane in the middle of the section on the left side. For the purposes of data extraction, the shoulder of the merging lane is also considered a travel lane since some vehicles illegally use it as an extended on-ramp to pass other drivers (see I395_ref_image.png for details). The cameras captured continuous footage during the morning rush hour (8:30 AM-10:30 AM ET) on a sunny day. During this period, vehicles equipped with SAE Level 2 automation were deployed to travel through the designated section to capture the impact of SAE Level 2-equipped vehicles on adjacent vehicles and their behavior in congested areas, particularly in complex merging sections. These vehicles are indicated in the dataset.\n\nAs part of this dataset, the following files were provided:\n<ul><li>I395-final.csv contains the numerical data to be used for analysis that includes vehicle level trajectory data at every 0.1 second. Vehicle type, width, and length are provided with instantaneous location, speed, and acceleration data. All distance measurements (width, length, location) were converted from pixels to meters using the following conversion factor: 1 pixel = 0.3-meter conversion.</li>\n<li>I395_ref_image.png is the aerial reference image that defines the geographic region and the associated roadway segments.</li>\n<li>I395_boundaries.csv contains the coordinates that define the roadway segments (n=X). The columns \"x1\" to \"x5\" represent the horizontal pi","distribution":[{"@type":"dcat:Distribution","describedBy":"https://data.transportation.gov/api/views/97n2-kuqi/columns.json","describedByType":"application/json","downloadURL":"https://data.transportation.gov/api/v3/views/97n2-kuqi/query.json?accessType=DOWNLOAD","mediaType":"application/json"},{"@type":"dcat:Distribution","describedBy":"https://data.transportation.gov/api/views/97n2-kuqi/columns.xml","describedByType":"application/xml","downloadURL":"https://data.transportation.gov/api/v3/views/97n2-kuqi/query.xml?accessType=DOWNLOAD","mediaType":"application/xml"},{"@type":"dcat:Distribution","downloadURL":"https://data.transportation.gov/api/v3/views/97n2-kuqi/export.csv?accessType=DOWNLOAD","mediaType":"text/csv"}],"identifier":"https://data.transportation.gov/api/views/97n2-kuqi","issued":"2024-11-04","keyword":["aerial videography","automated vehicles","human-automated vehicle interactions","infrastructure-based videography","intelligent transportation systems (its)","its joint program office (jpo)","multi-modal trajectories","tgsim","third generation simulation","vehicle trajectory data"],"landingPage":"https://data.transportation.gov/d/97n2-kuqi","license":"http://www.usa.gov/publicdomain/label/1.0/","modified":"2026-09-02","programCode":["021:042"],"publisher":{"@type":"org:Organization","name":"Federal Highway Administration"},"spatial":"I-90/I94 in Chicago, IL; I-294 near Hinsdale, IL; I-395 in Washington DC; George Washington University Campus, Washington DC (Foggy Bottom)","theme":["Automobiles"],"title":"Third Generation Simulation Data (TGSIM) I-395 Trajectories"},"description":"The main dataset is a 232 MB file of trajectory data (I395-final.csv) that contains position, speed, and acceleration data for non-automated passenger cars, trucks, buses, and automated vehicles on an expressway within an urban environment. 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Lane -5 corresponds to the area between \u201cx1\u201d and \u201cx2\u201d, and so forth to the rightmost lane, which is defined by the area to the right of \u201cx5\u201d (Lane -2). Lane -1 refers to vehicles that go onto the shoulder of the merging lane (Lane -2), which are manually separated by watching the videos.\n\nThis dataset was collected as part of the Third Generation Simulation Data (TGSIM): A Closer Look at the Impacts of Automated Driving Systems on Human Behavior project. During the project, six trajectory datasets capable of characterizing human-automated vehicle interactions under a diverse set of scenarios in highway and city environments were collected and processed. For more information, see the project report found here: https://rosap.ntl.bts.gov/view/dot/74647. This dataset, which was one of the six collected as part of the TGSIM project, contains data collected from six 4K cameras mounted on tripods, positioned on three overpasses along I-395 in Washington, D.C. The cameras captured distinct segments of the highway, and their combined overlapping and non-overlapping footage resulted in a continuous trajectory for the entire section covering 0.5 km. This section covers a major weaving/mandatory lane-changing between L'Enfant Plaza and 4th Street SW, with three lanes in the eastbound direction and a major on-ramp on the left side. In addition to the on-ramp, the section covers an off-ramp on the right side. The expressway includes one diverging lane at the beginning of the section on the right side and one merging lane in the middle of the section on the left side. For the purposes of data extraction, the shoulder of the merging lane is also considered a travel lane since some vehicles illegally use it as an extended on-ramp to pass other drivers (see I395_ref_image.png for details). The cameras captured continuous footage during the morning rush hour (8:30 AM-10:30 AM ET) on a sunny day. During this period, vehicles equipped with SAE Level 2 automation were deployed to travel through the designated section to capture the impact of SAE Level 2-equipped vehicles on adjacent vehicles and their behavior in congested areas, particularly in complex merging sections. These vehicles are indicated in the dataset.\n\nAs part of this dataset, the following files were provided:\n<ul><li>I395-final.csv contains the numerical data to be used for analysis that includes vehicle level trajectory data at every 0.1 second. Vehicle type, width, and length are provided with instantaneous location, speed, and acceleration data. 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This web portal is built using the github repository at https://github.com/usnistgov/SEA-DATA.\nThe purpose of the National Advanced Spectrum and Communications Test Network (NASCTN) Citizens Broadband Radio Service (CBRS) Sharing Ecosystem Assessment (SEA) project is to provide data-driven insight into the CBRS sharing ecosystem\u2019s effectiveness between commercial and Department of Defense (DoD) incumbent systems, and to track changes in the spectrum environment over time. CBRS is the \u201cfirst of a kind\u201d nationwide shared spectrum ecosystem in the 3550-3700 MHz band. The implementation of this project included the installation of sensor systems at selected sites on the east and the west coast of the United States, along with a control and prototyping system in Boulder, Colorado. This data provides time and frequency selective power measurements from 3530 MHz -3710 MHz from summer 2024 to summer of 2026. This data is targeted at the commercial, military and civilian stakeholders of Citizen's Broadband Radio Service (CBRS) that would benefit from in-depth real time and longitudinal analysis of a shared spectrum environment. These data were collected with sensors running the IEEE 802.15.22.3 Spectrum Characterization and Occupancy Sensing (SCOS) sensor system. In addition, the data is formatted and saved using  SigMF (signal metadata format). This project was a collaboration between NIST, NTIA / ITS, NASA and MITRE.","distribution":[{"accessURL":"https://github.com/usnistgov/SEA-DATA","description":"The github repository that is used to build the nist.pages site.","format":"github repository","title":"SEA-Data Web Portal Github Repository"},{"accessURL":"https://pages.nist.gov/SEA-DATA/","description":"A static website describing how to access data from the NASCTN CBRS SEA program.","format":"html","title":"NASCTN CBRS SEA DATA INSTRUCTIONS"}],"identifier":"ark:/88434/mds2-4219","issued":"2026-06-24","keyword":["CBRS","ESC","NASCTN","Naval Radar","RF","SAS","Wireless"],"landingPage":"https://data.nist.gov/od/id/mds2-4219","language":["en"],"license":"https://www.nist.gov/open/license","modified":"2026-06-01 00:00:00","programCode":["006:045"],"publisher":{"@type":"org:Organization","name":"National Institute of Standards and Technology"},"references":["https://nvlpubs.nist.gov/nistpubs/TechnicalNotes/NIST.TN.2359.pdf","https://www.mitre.org/sites/default/files/2026-01/PR-25-3159-spectrum-monitoring-sensor-radio-service-assessment.pdf"],"theme":["Advanced Communications:Wireless (RF)"],"title":"SEA-DATA Web Portal"},"description":"Data Access Instructions for The NASCTN CBRS SEA program. This web portal is built using the github repository at https://github.com/usnistgov/SEA-DATA.\nThe purpose of the National Advanced Spectrum and Communications Test Network (NASCTN) Citizens Broadband Radio Service (CBRS) Sharing Ecosystem Assessment (SEA) project is to provide data-driven insight into the CBRS sharing ecosystem\u2019s effectiveness between commercial and Department of Defense (DoD) incumbent systems, and to track changes in the spectrum environment over time. CBRS is the \u201cfirst of a kind\u201d nationwide shared spectrum ecosystem in the 3550-3700 MHz band. The implementation of this project included the installation of sensor systems at selected sites on the east and the west coast of the United States, along with a control and prototyping system in Boulder, Colorado. This data provides time and frequency selective power measurements from 3530 MHz -3710 MHz from summer 2024 to summer of 2026. 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While conventional treatments predict two symmetric sidebands from independent $m_J$ transitions, experiments have reported additional unexplained spectral features. We show that these arise from elliptical RF polarization, which coherently couples multiple magnetic sublevels and requires a full multi-level treatment.\nWe develop and diagonalize a Hamiltonian including all coupled m_J sublevels, predicting polarization-dependent degeneracies that produce two, three, or four resolved peaks. Using long-wavelength transitions and an anechoic environment we realize homogeneous RF fields that for the first time enable complete resolution of the m_J-dependent dressed states. We observe excellent agreement with theory as the RF ellipticity is varied.\nThese results demonstrate that RF polarization fundamentally modifies Autler\u2013Townes spectra and provide a consistent framework for interpreting magnetic-sublevel structure, with implications for Rydberg-based RF electrometry and polarimetry.","distribution":[{"downloadURL":"https://data.nist.gov/od/ds/mds2-4157/4157_README.txt","mediaType":"text/plain","title":"readme"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4157/Fig2.csv","mediaType":"text/csv","title":"Figure 2"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4157/Fig3.csv","mediaType":"text/csv","title":"Figure 3"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4157/Fig4.csv","mediaType":"text/csv","title":"Figure 4"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4157/Fig5.csv","mediaType":"text/csv","title":"Figure 5"}],"identifier":"ark:/88434/mds2-4157","issued":"2026-07-23","keyword":["Rydberg atoms","atomic physics","electric field","fields strength","receivers","volts/meter"],"landingPage":"https://data.nist.gov/od/id/mds2-4157","language":["en"],"license":"https://www.nist.gov/open/license","modified":"2026-04-13 00:00:00","programCode":["006:045"],"publisher":{"@type":"org:Organization","name":"National Institute of Standards and Technology"},"theme":["Physics:Atomic, molecular, and quantum","Physics:Spectroscopy"],"title":"Data associated with \"Resolving magnetic-sublevel structure in Rydberg Autler-Townes spectra with arbitrary RF polarization\""},"description":"We investigate the role of magnetic sublevels in Autler\u2013Townes spectra of Rydberg atoms driven by radio-frequency (RF) fields with arbitrary polarization. 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We observe excellent agreement with theory as the RF ellipticity is varied.\nThese results demonstrate that RF polarization fundamentally modifies Autler\u2013Townes spectra and provide a consistent framework for interpreting magnetic-sublevel structure, with implications for Rydberg-based RF electrometry and polarimetry.","distribution_titles":["readme","Figure 2","Figure 3","Figure 4","Figure 5"],"harvest_record":"https://catalog.data.gov/harvest_record/8e91ef57-be55-4f5d-bfb7-cb1137aeb050","harvest_record_raw":"https://catalog.data.gov/harvest_record/8e91ef57-be55-4f5d-bfb7-cb1137aeb050/raw","has_download":true,"has_spatial":false,"identifier":"ark:/88434/mds2-4157","keyword":["Rydberg atoms","atomic physics","electric field","fields strength","receivers","volts/meter"],"last_harvested_date":"2026-09-02T19:19:36.584464","organization":{"aliases":[""],"code_repo_exempt":false,"code_repo_url":null,"description":null,"id":"176f2a2d-ca9b-41f2-8df3-d93096ebdb85","logo":"https://raw.githubusercontent.com/GSA/logo/refs/heads/master/nist.png","name":"National Institute of Standards and Technology","organization_type":"Federal Government","slug":"nist"},"parent_identifier":null,"popularity":0,"publisher":"National Institute of Standards and Technology","slug":"data-associated-with-resolving-magnetic-sublevel-structure-in-rydberg-autler-townes-spectr","spatial_centroid":null,"spatial_shape":null,"theme":["Physics:Atomic, molecular, and quantum","Physics:Spectroscopy"],"title":"Data associated with \"Resolving magnetic-sublevel structure in Rydberg Autler-Townes spectra with arbitrary RF polarization\"","type":"dataset"},{"_score":2.99325,"_sort":[1788376775972,2.99325,0,"d034f1c1-28d0-4c2e-b434-41f027b9904a"],"dcat":{"@type":"dcat:Dataset","accessLevel":"public","accrualPeriodicity":"irregular","bureauCode":["006:55"],"contactPoint":{"fn":"Yamil Simon","hasEmail":"mailto:yamil.simon@nist.gov"},"description":"This mass spectrometry (MS) data set encompasses spectra of the extractables and leachables (E&L) of 100 polymer materials sourced from the Scientific Polymer Products Inc Polymer Samples Kit (see: SciPoly_PolymerSampleKit205_Items.xlsx). Extractions of these polymers were carried out using three HPLC-grade solvents of varying polarity (water, isopropanol, and hexane) with 10 mg polymer/mL solvent for 24 hours at 50 \u00b0C with shaking. To account for solvent volatility, extractions were carried out in 8 mL pressure tubes from Ace Glass Incorporated (Product #8648-25) (rated at 150 psig).\n\nExtraction solutions were subsequently analyzed using three ionization techniques: Electron Ionization (EI) with GC-MS and Electrospray Ionization (ESI) and Atmospheric Pressure Chemical Ionization (APCI) via LC-MS/MS on an Agilent QTOF 6530 and a Bruker timsTOF Pro 2, respectively.\n\nSeveral precautionary measures had to be taken following the extraction procedure. Extracts were centrifuged and filtered using 0.45-micron syringe filters to prevent prohibitively large particles from interfering with chromatography and MS analysis. Moreover, a guard column was used before the LC column to avoid contamination. As such, pressure build-up would often be a concern, so the LC and guard column had to be thoroughly flushed after each analysis batch.\n\nThousands of spectra were processed using in-house software, generating lists of identifications using the most recent versions of the NIST MS libraries via both direct and hybrid search methods. Some monomers were detected under the given extraction conditions, and many plastic additives (e.g., plasticizers, antioxidants, and processing agents) could be identified; some common examples found in many of the polymer standards include oleamide and palmitamide. High-quality unidentified spectra obtained from the extracts are included in a library of annotated recurrent unidentified spectra (ARUS).\n\nLC Chromatographic Separation Method: LC runs were performed using reversed-phase chromatography with an ACQUITY UPLC CSH C18 column (130 \u00c5 (13.0 nm), 1.7 \u00b5m, 2.1 mm x 100 mm), mobile phase A: water, and mobile phase B: acetonitrile (both mobile phases containing 0.1 % formic acid). The chromatographic separation method was as follows: injection volume: 10 \u00b5L, column temperature: 35\u00b0C, flow rate: 0.400 mL/min, and gradient: initial condition of 1.00% B, hold for 1.00 min, linear ramp to 80.00% B in 8.00 min, linear ramp to 99.00% B in 3.00 min, hold for 1.50 min, linear ramp to 1.00% B in 0.50 min, hold for 1.00 min. GC Chromatographic Separation Method: Spectra were obtained using an Agilent 5977B instrument, with GC runs performed using a Restek Rxi-5Sil MS GC Capillary Column (15 m x 250 \u00b5m x 0.25 \u00b5m) under 2 mL/min He flow. The initial oven temperature was 40\u00b0C (held for 3 min), with a ramp rate of 20\u00b0C/min, final temperature of 320\u00b0C, and final hold time of 3.75 min. \n\nReferences:\n\nBerthelette, K.; Walter, T. H. Column screening for the UPLC separation of plastic additives as part of extractables and leachables workflows; 720006777EN; Waters Corporation, MA, USA, 2020.\n\nLee, P. J.; Di Gioia, A. J. Rapid analysis of 25 common polymer additives; 720002488EN; Waters Corporation, Milford, MA, USA, 2008.\n\nSim\u00f3n-Manso, Y.; Erisman, E. P.; Mak, T. D.; Burke, M. C.; Zuber, A.; Yang, X.; Liang, Y.; Neta, P.; Bukhari, T.; Williams, A. J.; et al. NIST Mass Spectral Libraries in the Context of the Circular Economy of Plastics. J Am Soc Mass Spectrom 2025, 36 (2), 439\u2013445. DOI: 10.1021/jasms.4c00349.\n","distribution":[{"description":"The file contains a description of the dataset directory.","downloadURL":"https://data.nist.gov/od/ds/mds2-4147/4147_README.txt","format":".txt","mediaType":"text/plain","title":"README"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4147/GC_MS_single_quad.zip","mediaType":"application/zip","title":"GC_MS_single_quad"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4147/QTOF_ESI.zip","mediaType":"application/zip","title":"QTOF_ESI"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4147/SciPoly_PolymerSampleKit205_Items.xlsx","mediaType":"application/vnd.openxmlformats-officedocument.spreadsheetml.sheet","title":"SciPoly_PolymerSampleKit205_Items"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4147/timsTOF_APCI.zip","mediaType":"application/zip","title":"timsTOF_APCI"}],"identifier":"ark:/88434/mds2-4147","issued":"2026-05-13","keyword":["APCI-LC-MS/MS","ESI-LC-MS/MS","GC-MS","extractables and leachables","ion mobility","mass spectrometry","plastic-related compounds","plastics","polymers","tandem mass spectrometry"],"landingPage":"https://data.nist.gov/od/id/mds2-4147","language":["en"],"license":"https://www.nist.gov/open/license","modified":"2026-03-19 00:00:00","programCode":["006:045"],"publisher":{"@type":"org:Organization","name":"National Institute of Standards and Technology"},"theme":["Chemistry","Chemistry:Analytical chemistry","Environment"],"title":"LC-MS/MS and GC-MS Measurements of Extractables and Leachables (E&L) from Polymeric Materials"},"description":"This mass spectrometry (MS) data set encompasses spectra of the extractables and leachables (E&L) of 100 polymer materials sourced from the Scientific Polymer Products Inc Polymer Samples Kit (see: SciPoly_PolymerSampleKit205_Items.xlsx). Extractions of these polymers were carried out using three HPLC-grade solvents of varying polarity (water, isopropanol, and hexane) with 10 mg polymer/mL solvent for 24 hours at 50 \u00b0C with shaking. To account for solvent volatility, extractions were carried out in 8 mL pressure tubes from Ace Glass Incorporated (Product #8648-25) (rated at 150 psig).\n\nExtraction solutions were subsequently analyzed using three ionization techniques: Electron Ionization (EI) with GC-MS and Electrospray Ionization (ESI) and Atmospheric Pressure Chemical Ionization (APCI) via LC-MS/MS on an Agilent QTOF 6530 and a Bruker timsTOF Pro 2, respectively.\n\nSeveral precautionary measures had to be taken following the extraction procedure. Extracts were centrifuged and filtered using 0.45-micron syringe filters to prevent prohibitively large particles from interfering with chromatography and MS analysis. Moreover, a guard column was used before the LC column to avoid contamination. As such, pressure build-up would often be a concern, so the LC and guard column had to be thoroughly flushed after each analysis batch.\n\nThousands of spectra were processed using in-house software, generating lists of identifications using the most recent versions of the NIST MS libraries via both direct and hybrid search methods. Some monomers were detected under the given extraction conditions, and many plastic additives (e.g., plasticizers, antioxidants, and processing agents) could be identified; some common examples found in many of the polymer standards include oleamide and palmitamide. High-quality unidentified spectra obtained from the extracts are included in a library of annotated recurrent unidentified spectra (ARUS).\n\nLC Chromatographic Separation Method: LC runs were performed using reversed-phase chromatography with an ACQUITY UPLC CSH C18 column (130 \u00c5 (13.0 nm), 1.7 \u00b5m, 2.1 mm x 100 mm), mobile phase A: water, and mobile phase B: acetonitrile (both mobile phases containing 0.1 % formic acid). The chromatographic separation method was as follows: injection volume: 10 \u00b5L, column temperature: 35\u00b0C, flow rate: 0.400 mL/min, and gradient: initial condition of 1.00% B, hold for 1.00 min, linear ramp to 80.00% B in 8.00 min, linear ramp to 99.00% B in 3.00 min, hold for 1.50 min, linear ramp to 1.00% B in 0.50 min, hold for 1.00 min. GC Chromatographic Separation Method: Spectra were obtained using an Agilent 5977B instrument, with GC runs performed using a Restek Rxi-5Sil MS GC Capillary Column (15 m x 250 \u00b5m x 0.25 \u00b5m) under 2 mL/min He flow. The initial oven temperature was 40\u00b0C (held for 3 min), with a ramp rate of 20\u00b0C/min, final temperature of 320\u00b0C, and final hold time of 3.75 min. \n\nReferences:\n\nBerthelette, K.; Walter, T. H. Column screening for the UPLC separation of plastic additives as part of extractables and leachables workflows; 720006777EN; Waters Corporation, MA, USA, 2020.\n\nLee, P. J.; Di Gioia, A. J. Rapid analysis of 25 common polymer additives; 720002488EN; Waters Corporation, Milford, MA, USA, 2008.\n\nSim\u00f3n-Manso, Y.; Erisman, E. P.; Mak, T. D.; Burke, M. C.; Zuber, A.; Yang, X.; Liang, Y.; Neta, P.; Bukhari, T.; Williams, A. J.; et al. NIST Mass Spectral Libraries in the Context of the Circular Economy of Plastics. J Am Soc Mass Spectrom 2025, 36 (2), 439\u2013445. 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In this work, we demonstrate a solution to this problem by using a frequency multiplier to drive the qubit with room-temperature control pulses at half or one third of the qubit frequency fQB. The control pulses are up-converted inside the cryogenic environment using a frequency multiplier based on a high-kinetic inductance nonlinear transmission line. We evaluated the success of the up-conversion technique by comparing the randomized benchmarking error-per-gate metrics to that of a standard direct qubit driving technique. The fQB/2 drive technique achieved error rates consistent with the direct drive, with a minimum error-per-gate of 3.5x10\u22123\u00b10.4x10\u22123. The fQB/3 drive technique resulted in a minimum error per gate of 7.6x10\u22123\u00b10.81x10\u22123. While this demonstration is based around a fQB = 4.836 GHz qubit so that a direct drive comparison is possible, this technique will allow higher-frequency qubits to be tested using existing radio-frequency (RF) infrastructure.","distribution":[{"downloadURL":"https://data.nist.gov/od/ds/mds2-4118/4118_README.txt","mediaType":"text/plain","title":"4118_README"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4118/fig2.json","mediaType":"application/json","title":"fig2"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4118/fig3.json","mediaType":"application/json","title":"fig3"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4118/fig5_left.txt","mediaType":"text/plain","title":"fig5_left"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4118/fig5_right.txt","mediaType":"text/plain","title":"fig5_right"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4118/fig6_direct_drive.txt","mediaType":"text/plain","title":"fig6_direct_drive"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4118/fig6_doubler.txt","mediaType":"text/plain","title":"fig6_doubler"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4118/fig6_tripler.txt","mediaType":"text/plain","title":"fig6_tripler"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4118/fig7.json","mediaType":"application/json","title":"fig7"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4118/fig8.json","mediaType":"application/json","title":"fig8"}],"identifier":"ark:/88434/mds2-4118","issued":"2026-05-05","keyword":["Frequency conversion.","Superconductors","kinetic inductance"],"landingPage":"https://data.nist.gov/od/id/mds2-4118","language":["en"],"license":"https://www.nist.gov/open/license","modified":"2026-02-26 00:00:00","programCode":["006:045"],"publisher":{"@type":"org:Organization","name":"National Institute of Standards and Technology"},"theme":["Electronics:Superconducting electronics"],"title":"Superconducting Qubit Control Using Cryogenic Frequency Conversion"},"description":"Dataset for the APL paper \"Superconducting Qubit Control Using Cryogenic Frequency Conversion\".\n\nAbstract:\nExpanding to higher qubit frequencies introduces the challenge of routing > 20 GHz signals into a dilution refrigerator without adding excess thermal load or frequency-dependent loss. 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For large (sparse) feature matrices, especially ones with binary-valued entries, techniques to figure out the underlying structure of the feature space are widely varied, and different communities have widely different practices and assumptions for what is an appropriate approach. 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From numerical simulations of SWAP using our laser beam geometry, we find that SWAP provides greater cooling than triangle wave frequency modulation despite the complex polarization environment of a grating MOT. The simulation is confirmed by experimental results, which show a factor of two improvement in transfer efficiency between a dipole-allowed transition grating MOT and an intercombination transition grating MOT.\nThe data show that the intercombination line grating MOT can trap up to three million strontium atoms at an average temperature of 4.9 microkelvin with a lifetime of approximately 0.7 seconds.\n\nInstructions on reproducing the figures in the manuscript are included in 4097_README.txt.","distribution":[{"description":"README file for the .zip archive.","downloadURL":"https://data.nist.gov/od/ds/mds2-4097/4097_README.txt","format":".txt","mediaType":"text/plain","title":"README"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-4097/figure_generation_data.zip","mediaType":"application/zip","title":"figure_generation_data"}],"identifier":"ark:/88434/mds2-4097","issued":"2026-05-21","keyword":["atomic physics","laser cooling","quantum physics"],"landingPage":"https://data.nist.gov/od/id/mds2-4097","language":["en"],"license":"https://www.nist.gov/open/license","modified":"2026-02-09 00:00:00","programCode":["006:045"],"publisher":{"@type":"org:Organization","name":"National Institute of Standards and Technology"},"references":["https://doi.org/10.48550/arXiv.2602.06230"],"theme":["Physics:Atomic, molecular, and quantum"],"title":"Data associated with \"Sawtooth wave adiabatic passage in a grating magneto-optical trap\""},"description":"Numerical values of data points and figure generation scripts for manuscript \"Sawtooth wave adiabatic passage in a grating magneto-optical trap\" submitted for publication and available on ArXiv (2602.06230).\n\nThis data set demonstrates sawtooth wave adiabatic passage (SWAP) in a grating magneto-optical trap (MOT) operating on the intercombination transition of neutral strontium. From numerical simulations of SWAP using our laser beam geometry, we find that SWAP provides greater cooling than triangle wave frequency modulation despite the complex polarization environment of a grating MOT. The simulation is confirmed by experimental results, which show a factor of two improvement in transfer efficiency between a dipole-allowed transition grating MOT and an intercombination transition grating MOT.\nThe data show that the intercombination line grating MOT can trap up to three million strontium atoms at an average temperature of 4.9 microkelvin with a lifetime of approximately 0.7 seconds.\n\nInstructions on reproducing the figures in the manuscript are included in 4097_README.txt.","distribution_titles":["README","figure_generation_data"],"harvest_record":"https://catalog.data.gov/harvest_record/1d97f4e8-b1a1-4501-928f-f65b9bfb5aef","harvest_record_raw":"https://catalog.data.gov/harvest_record/1d97f4e8-b1a1-4501-928f-f65b9bfb5aef/raw","has_download":true,"has_spatial":false,"identifier":"ark:/88434/mds2-4097","keyword":["atomic physics","laser cooling","quantum physics"],"last_harvested_date":"2026-09-02T19:19:32.937114","organization":{"aliases":[""],"code_repo_exempt":false,"code_repo_url":null,"description":null,"id":"176f2a2d-ca9b-41f2-8df3-d93096ebdb85","logo":"https://raw.githubusercontent.com/GSA/logo/refs/heads/master/nist.png","name":"National Institute of Standards and Technology","organization_type":"Federal Government","slug":"nist"},"parent_identifier":null,"popularity":0,"publisher":"National Institute of Standards and Technology","slug":"data-associated-with-sawtooth-wave-adiabatic-passage-in-a-grating-magneto-optical-trap","spatial_centroid":null,"spatial_shape":null,"theme":["Physics:Atomic, molecular, and quantum"],"title":"Data associated with \"Sawtooth wave adiabatic passage in a grating magneto-optical trap\"","type":"dataset"},{"_score":22.582508,"_sort":[1788376769721,22.582508,0,"67c7a7c9-20c0-4738-835b-7c2aacdfa5f3"],"dcat":{"@type":"dcat:Dataset","accessLevel":"public","accrualPeriodicity":"irregular","bureauCode":["006:55"],"contactPoint":{"fn":"Mohamed Hany","hasEmail":"mailto:mohamed.hany@nist.gov"},"description":"In this paper, we present a standardized, repeatable test approach that replicates key features of measured industrial environments in a fully-characterized hybrid test chamber. The hybrid chamber consists of an anechoic chamber along with movable metallic spheres that provide discrete reconfigurable multipath components. The chamber is characterized by a synthetic-aperture system providing a reference measurement that captures the non-idealities of the chamber along with the intended spatial multipath, completing characterization of the test environment. A key feature of our approach is the propagation of correlated uncertainties through to the final system response \u2013 including uncertainties specific to synthetic apertures such as cable bending due to scanning and inexact positioner locations. The uncertainty analysis provides statistically accurate knowledge of the environment, allowing separation of measurement errors from errors related to the device or system under test. We have also extracted three exemplar channels that capture key features of a work-cell-sized industrial environment from measurements made with the same synthetic 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channel; industrial internet of things; industrial wireless systems; millimeter-wave wireless; synthetic aperture; wireless system."],"landingPage":"https://data.nist.gov/od/id/mds2-4030","language":["en"],"license":"https://www.nist.gov/open/license","modified":"2025-12-03 00:00:00","programCode":["006:045"],"publisher":{"@type":"org:Organization","name":"National Institute of Standards and Technology"},"theme":["Advanced Communications:Advanced Communications"],"title":"Standardized Approach for Assessing Wireless IoT Devices in Millimeter-Wave Industrial Work-Cell Channels"},"description":"In this paper, we present a standardized, repeatable test approach that replicates key features of measured industrial environments in a fully-characterized hybrid test chamber. The hybrid chamber consists of an anechoic chamber along with movable metallic spheres that provide discrete reconfigurable multipath components. The chamber is characterized by a synthetic-aperture system providing a reference measurement that captures the non-idealities of the chamber along with the intended spatial multipath, completing characterization of the test environment. A key feature of our approach is the propagation of correlated uncertainties through to the final system response \u2013 including uncertainties specific to synthetic apertures such as cable bending due to scanning and inexact positioner locations. The uncertainty analysis provides statistically accurate knowledge of the environment, allowing separation of measurement errors from errors related to the device or system under test. 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This data will be used to develop software solutions for detecting that trigger behavior in the trained AI models.","distribution_titles":["rl-safetygymnasium-oct2024-test"],"harvest_record":"https://catalog.data.gov/harvest_record/79dae698-3893-4218-b778-f33a54e498a3","harvest_record_raw":"https://catalog.data.gov/harvest_record/79dae698-3893-4218-b778-f33a54e498a3/raw","has_download":false,"has_spatial":false,"identifier":"ark:/88434/mds2-3899","keyword":["Trojan Detection; Artificial Intelligence; AI; Machine Learning; Adversarial Machine Learning;"],"last_harvested_date":"2026-09-02T19:19:20.089417","organization":{"aliases":[""],"code_repo_exempt":false,"code_repo_url":null,"description":null,"id":"176f2a2d-ca9b-41f2-8df3-d93096ebdb85","logo":"https://raw.githubusercontent.com/GSA/logo/refs/heads/master/nist.png","name":"National Institute of Standards and Technology","organization_type":"Federal Government","slug":"nist"},"parent_identifier":null,"popularity":0,"publisher":"National Institute of Standards and Technology","slug":"trojan-detection-software-challenge-rl-safetygymnasium-oct2024-test","spatial_centroid":null,"spatial_shape":null,"theme":["Information Technology:Cybersecurity","Information Technology:Software research"],"title":"Trojan Detection Software Challenge - rl-safetygymnasium-oct2024-test","type":"dataset"},{"_score":21.787785,"_sort":[1788376754340,21.787785,1,"7c917a2d-7d31-4492-815f-a7b8d43b1439"],"dcat":{"@type":"dcat:Dataset","accessLevel":"public","bureauCode":["006:55"],"contactPoint":{"fn":"Junxiao Shi","hasEmail":"mailto:junxiao.shi@nist.gov"},"description":"This is a set of scripts to deploy and control 5G network.\nIt is primarily useful for running an emulated 5G network in Docker Compose environment.","distribution":[{"accessURL":"https://github.com/usnistgov/5gdeploy","title":"GitHub repository"}],"identifier":"ark:/88434/mds2-3794","issued":"2025-04-10","keyword":["3GPP","5G core network","5G network","Docker Compose"],"language":["en"],"license":"https://www.nist.gov/open/license","modified":"2025-04-02 00:00:00","programCode":["006:045"],"publisher":{"@type":"org:Organization","name":"National Institute of Standards and Technology"},"theme":["Information Technology:Mobile","Information Technology:Networking"],"title":"5gdeploy: 5G Core Deployment Helper"},"description":"This is a set of scripts to deploy and control 5G network.\nIt is primarily useful for running an emulated 5G network in Docker Compose environment.","distribution_titles":["GitHub repository"],"harvest_record":"https://catalog.data.gov/harvest_record/16e5b218-3519-4961-a020-7413e2989f10","harvest_record_raw":"https://catalog.data.gov/harvest_record/16e5b218-3519-4961-a020-7413e2989f10/raw","has_download":false,"has_spatial":false,"identifier":"ark:/88434/mds2-3794","keyword":["3GPP","5G core network","5G network","Docker Compose"],"last_harvested_date":"2026-09-02T19:19:14.340266","organization":{"aliases":[""],"code_repo_exempt":false,"code_repo_url":null,"description":null,"id":"176f2a2d-ca9b-41f2-8df3-d93096ebdb85","logo":"https://raw.githubusercontent.com/GSA/logo/refs/heads/master/nist.png","name":"National Institute of Standards and Technology","organization_type":"Federal Government","slug":"nist"},"parent_identifier":null,"popularity":1,"publisher":"National Institute of Standards and Technology","slug":"5gdeploy-5g-core-deployment-helper","spatial_centroid":null,"spatial_shape":null,"theme":["Information Technology:Mobile","Information Technology:Networking"],"title":"5gdeploy: 5G Core Deployment Helper","type":"dataset"},{"_score":15.041035,"_sort":[1788376752188,15.041035,2,"2c9d9995-294f-4529-91f9-36f59e0c8647"],"dcat":{"@type":"dcat:Dataset","accessLevel":"public","accrualPeriodicity":"R/PT1S","bureauCode":["006:55"],"contactPoint":{"fn":"Thomas Roth","hasEmail":"mailto:thomas.roth@nist.gov"},"description":"The Internet of Things (IoT) is comprised of networks of physical, computational, and human components that coordinate to fulfill time-sensitive functions in a shared operating environment. Development and testing of IoT systems often utilizes modeling and simulation, whether to analyze potential performance gains of new technologies or develop robust digital twins to support future operations and maintenance. However, the complexity and scale of IoT means that individual simulators are often inadequate to simulate the real-world dynamics of such systems, and simulators must be combined with other software or hardware.\n\nThe National Institute of Standards and Technology (NIST) has developed a software module that extends the ns-3 network simulator with a new capability to communicate with external software and hardware at runtime. This software facilitates the development of co-simulations where ns-3 models can synchronize and exchange data with external processes to develop higher-fidelity simulations. The software is open-source and available on the NIST GitHub.","distribution":[{"accessURL":"https://github.com/usnistgov/ns3-cosim","description":"A GitHub page that includes the documentation and source code for the software.","format":"GitHub Software Repository","title":"ns-3 Gateway Software Repository"}],"identifier":"ark:/88434/mds2-3738","issued":"2025-03-31","keyword":["automated vehicles","co-simulation","cyber-physical systems","internet of things","network simulation","ns-3","software"],"landingPage":"https://data.nist.gov/od/id/mds2-3738","language":["en"],"license":"https://www.nist.gov/open/license","modified":"2025-02-18 00:00:00","programCode":["006:045"],"publisher":{"@type":"org:Organization","name":"National Institute of Standards and Technology"},"theme":["Advanced Communications:Wireless (RF)","Information Technology:Cyber-physical systems","Information Technology:Internet of Things","Information Technology:Networking","Transportation:Automotive"],"title":"Gateway for Co-Simulation using ns-3"},"description":"The Internet of Things (IoT) is comprised of networks of physical, computational, and human components that coordinate to fulfill time-sensitive functions in a shared operating environment. Development and testing of IoT systems often utilizes modeling and simulation, whether to analyze potential performance gains of new technologies or develop robust digital twins to support future operations and maintenance. However, the complexity and scale of IoT means that individual simulators are often inadequate to simulate the real-world dynamics of such systems, and simulators must be combined with other software or hardware.\n\nThe National Institute of Standards and Technology (NIST) has developed a software module that extends the ns-3 network simulator with a new capability to communicate with external software and hardware at runtime. This software facilitates the development of co-simulations where ns-3 models can synchronize and exchange data with external processes to develop higher-fidelity simulations. The software is open-source and available on the NIST GitHub.","distribution_titles":["ns-3 Gateway Software Repository"],"harvest_record":"https://catalog.data.gov/harvest_record/15b3c00a-24e1-44e2-9629-b5a704ad4bb6","harvest_record_raw":"https://catalog.data.gov/harvest_record/15b3c00a-24e1-44e2-9629-b5a704ad4bb6/raw","has_download":false,"has_spatial":false,"identifier":"ark:/88434/mds2-3738","keyword":["automated vehicles","co-simulation","cyber-physical systems","internet of things","network simulation","ns-3","software"],"last_harvested_date":"2026-09-02T19:19:12.188135","organization":{"aliases":[""],"code_repo_exempt":false,"code_repo_url":null,"description":null,"id":"176f2a2d-ca9b-41f2-8df3-d93096ebdb85","logo":"https://raw.githubusercontent.com/GSA/logo/refs/heads/master/nist.png","name":"National Institute of Standards and Technology","organization_type":"Federal Government","slug":"nist"},"parent_identifier":null,"popularity":2,"publisher":"National Institute of Standards and Technology","slug":"gateway-for-co-simulation-using-ns-3","spatial_centroid":null,"spatial_shape":null,"theme":["Advanced Communications:Wireless (RF)","Information Technology:Cyber-physical systems","Information Technology:Internet of Things","Information Technology:Networking","Transportation:Automotive"],"title":"Gateway for Co-Simulation using ns-3","type":"dataset"},{"_score":8.908609,"_sort":[1788376751219,8.908609,6,"f907a22c-7304-4e4c-b7d4-dc921d42c75a"],"dcat":{"@type":"dcat:Dataset","accessLevel":"public","bureauCode":["006:55"],"contactPoint":{"fn":"Justyna Zwolak","hasEmail":"mailto:justyna.zwolak@nist.gov"},"description":"The dataset underlying the figures in the manuscript is \"Modular Autonomous Virtualization System for Two-Dimensional Semiconductor Quantum Dot Arrays.\"\n\nAbstract of the paper: Arrays of gate-defined semiconductor quantum dots are among the leading candidates for building scalable quantum processors. High-fidelity initialization, control, and readout of spin qubit registers require exquisite and targeted control over key Hamiltonian parameters that define the electrostatic environment. However, due to the tight gate pitch, capacitive crosstalk between gates hinders independent tuning of chemical potentials and interdot couplings. While virtual gates offer a practical solution, determining all the required cross-capacitance matrices accurately and efficiently in large quantum dot registers is an open challenge. Here, we establish a Modular Automated Virtualization System (MAViS) -- a general and modular framework for autonomously constructing a complete stack of multi-layer virtual gates in real time. Our method employs machine learning techniques to rapidly extract features from two-dimensional charge stability diagrams. We then utilize computer vision and regression models to self-consistently determine all relative capacitive couplings necessary for virtualizing plunger and barrier gates in both low- and high-tunnel-coupling regimes. Using MAViS, we successfully demonstrate accurate virtualization of a dense two-dimensional array comprising ten quantum dots defined in a high-quality Ge/SiGe heterostructure. Our work offers an elegant and practical solution for the efficient control of large-scale semiconductor quantum dot systems.\n\nData description: Each figure folder contains a complete set of files necessary to reproduce figures, including Jupyter Notebooks with the figure source code, Adobe Illustrator, and pre-processed data files (hdf5 and pkl). The complete set of all raw data files used in this study is available at Zenodo. [doi: 10.5281/zenodo.14173838].\n\nAcknowledgments: This research was sponsored in part by the Army Research Office (ARO) under Awards No. W911NF-23-1-0110 and W911NF-23-1-0258. We acknowledge support from the European Union through the IGNITE project with grant agreement No. 101069515 and from the Dutch Research Council (NWO) via the National Growth Fund program Quantum Delta NL (Grant No. NGF.1582.22.001). The views, conclusions, and recommendations contained in this paper are those of the authors and are not necessarily endorsed nor should they be interpreted as representing the official policies, either expressed or implied, of the Army Research Office (ARO) or the U.S. Government. The U.S. Government is authorized to reproduce and distribute reprints for Government purposes notwithstanding any copyright noted herein. Any mention of commercial products is for information only; it does not imply recommendation or endorsement by the National Institute of Standards and Technology.","distribution":[{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-1.zip","mediaType":"application/zip","title":"Figure-1"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-2.zip","mediaType":"application/zip","title":"Figure-2"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-3.zip","mediaType":"application/zip","title":"Figure-3"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-4.zip","mediaType":"application/zip","title":"Figure-4"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-5.zip","mediaType":"application/zip","title":"Figure-5"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-SM1.zip","mediaType":"application/zip","title":"Figure-SM1"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-SM2.zip","mediaType":"application/zip","title":"Figure-SM2"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-SM3.zip","mediaType":"application/zip","title":"Figure-SM3"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-SM4.zip","mediaType":"application/zip","title":"Figure-SM4"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-SM5.zip","mediaType":"application/zip","title":"Figure-SM5"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-SM6.zip","mediaType":"application/zip","title":"Figure-SM6"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-SM7.zip","mediaType":"application/zip","title":"Figure-SM7"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/Figure-SM8.zip","mediaType":"application/zip","title":"Figure-SM8"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3705/README.txt","mediaType":"text/plain","title":"README"}],"identifier":"ark:/88434/mds2-3705","issued":"2025-03-17","keyword":["2D arrays","autonomous control","germanium quantum dots","machine learning","quantum dots"],"language":["en"],"license":"https://www.nist.gov/open/license","modified":"2025-02-03 00:00:00","programCode":["006:045"],"publisher":{"@type":"org:Organization","name":"National Institute of Standards and Technology"},"references":["https://doi.org/10.48550/arXiv.2411.12516"],"theme":["Information Technology:Data and informatics","Mathematics and Statistics:Image and signal processing","Mathematics and Statistics:Numerical methods and software","Physics:Condensed matter","Physics:Quantum information science"],"title":"Figure files for \"Modular Autonomous Virtualization System for Two-Dimensional Semiconductor Quantum Dot Arrays\" submitted to Physical Review X"},"description":"The dataset underlying the figures in the manuscript is \"Modular Autonomous Virtualization System for Two-Dimensional Semiconductor Quantum Dot Arrays.\"\n\nAbstract of the paper: Arrays of gate-defined semiconductor quantum dots are among the leading candidates for building scalable quantum processors. 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We then utilize computer vision and regression models to self-consistently determine all relative capacitive couplings necessary for virtualizing plunger and barrier gates in both low- and high-tunnel-coupling regimes. Using MAViS, we successfully demonstrate accurate virtualization of a dense two-dimensional array comprising ten quantum dots defined in a high-quality Ge/SiGe heterostructure. Our work offers an elegant and practical solution for the efficient control of large-scale semiconductor quantum dot systems.\n\nData description: Each figure folder contains a complete set of files necessary to reproduce figures, including Jupyter Notebooks with the figure source code, Adobe Illustrator, and pre-processed data files (hdf5 and pkl). The complete set of all raw data files used in this study is available at Zenodo. [doi: 10.5281/zenodo.14173838].\n\nAcknowledgments: This research was sponsored in part by the Army Research Office (ARO) under Awards No. W911NF-23-1-0110 and W911NF-23-1-0258. We acknowledge support from the European Union through the IGNITE project with grant agreement No. 101069515 and from the Dutch Research Council (NWO) via the National Growth Fund program Quantum Delta NL (Grant No. NGF.1582.22.001). The views, conclusions, and recommendations contained in this paper are those of the authors and are not necessarily endorsed nor should they be interpreted as representing the official policies, either expressed or implied, of the Army Research Office (ARO) or the U.S. Government. The U.S. Government is authorized to reproduce and distribute reprints for Government purposes notwithstanding any copyright noted herein. Any mention of commercial products is for information only; it does not imply recommendation or endorsement by the National Institute of Standards and Technology.","distribution_titles":["Figure-1","Figure-2","Figure-3","Figure-4","Figure-5","Figure-SM1","Figure-SM2","Figure-SM3","Figure-SM4","Figure-SM5","Figure-SM6","Figure-SM7","Figure-SM8","README"],"harvest_record":"https://catalog.data.gov/harvest_record/7280205e-e86b-4879-b15f-cb0f896b964f","harvest_record_raw":"https://catalog.data.gov/harvest_record/7280205e-e86b-4879-b15f-cb0f896b964f/raw","has_download":true,"has_spatial":false,"identifier":"ark:/88434/mds2-3705","keyword":["2D arrays","autonomous control","germanium quantum dots","machine learning","quantum dots"],"last_harvested_date":"2026-09-02T19:19:11.219874","organization":{"aliases":[""],"code_repo_exempt":false,"code_repo_url":null,"description":null,"id":"176f2a2d-ca9b-41f2-8df3-d93096ebdb85","logo":"https://raw.githubusercontent.com/GSA/logo/refs/heads/master/nist.png","name":"National Institute of Standards and Technology","organization_type":"Federal Government","slug":"nist"},"parent_identifier":null,"popularity":6,"publisher":"National Institute of Standards and Technology","slug":"figure-files-for-modular-autonomous-virtualization-system-for-two-dimensional-semiconducto","spatial_centroid":null,"spatial_shape":null,"theme":["Information Technology:Data and informatics","Mathematics and Statistics:Image and signal processing","Mathematics and Statistics:Numerical methods and software","Physics:Condensed matter","Physics:Quantum information science"],"title":"Figure files for \"Modular Autonomous Virtualization System for Two-Dimensional Semiconductor Quantum Dot Arrays\" submitted to Physical Review X","type":"dataset"},{"_score":20.84819,"_sort":[1788376750223,20.84819,35,"a3ff116f-9b4b-46c5-ae8f-082bb819ea1a"],"dcat":{"@type":"dcat:Dataset","accessLevel":"public","accrualPeriodicity":"irregular","bureauCode":["006:55"],"contactPoint":{"fn":"Tony Wang","hasEmail":"mailto:tony.wang@nist.gov"},"description":"AgentDojo-Inspect is a codebase created by the U.S. AI Safety Institute to facilitate research into agent hijacking and defenses against said hijacking. Agent hijacking is a type of indirect prompt injection\u00a0[1] in which an attacker inserts malicious instructions into data that may be ingested by an AI agent, causing it to take unintended, harmful actions.\n\nAgentDojo-Inspect is a fork of the original AgentDojo repository [2], which was created by\u00a0researchers at ETH Zurich [3]. This fork extends the upstream AgentDojo in four key ways:\n\n1. It adds an Inspect bridge that allows AgentDojo evaluations to be run using the Inspect evaluations framework [4] (see below for more details).\n\n2. It fixes some bugs in the upstream AgentDojo's task suites (most of these fixes have been merged upstream). It also removes certain tasks that are of low quality.\n\n3. It adds new injection tasks in the Workspace environment that have to do with mass data exfiltration (these have since been merged upstream).\n\n4. It adds a new terminal environment and associated tasks that test for remote code execution vulnerabilities in this environment.\n\n[1] Greshake K, Abdelnabi S, Mishra S, Endres C, Holz T, Fritz M (2023) Not what you?ve signed up for: Compromising Real-World LLM-Integrated Applications with Indirect Prompt Injection (arXiv), arXiv:2302.12173. https://doi.org/10.48550/arXiv.2302.12173\n\n[2] Edoardo Debenedetti (2025) ethz-spylab/agentdojo. Available at https://github.com/ethz-spylab/agentdojo.\n\n[3] Debenedetti E, Zhang J, Balunovi? M, Beurer-Kellner L, Fischer M, Tram\u00e8r F (2024) AgentDojo: A Dynamic Environment to Evaluate Prompt Injection Attacks and Defenses for LLM Agents (arXiv), arXiv:2406.13352. https://doi.org/10.48550/arXiv.2406.13352\n\n[4] UK AI Safety Institute (2024) Inspect AI: Framework for Large Language Model\u00a0Evaluations. 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Agent hijacking is a type of indirect prompt injection\u00a0[1] in which an attacker inserts malicious instructions into data that may be ingested by an AI agent, causing it to take unintended, harmful actions.\n\nAgentDojo-Inspect is a fork of the original AgentDojo repository [2], which was created by\u00a0researchers at ETH Zurich [3]. This fork extends the upstream AgentDojo in four key ways:\n\n1. It adds an Inspect bridge that allows AgentDojo evaluations to be run using the Inspect evaluations framework [4] (see below for more details).\n\n2. It fixes some bugs in the upstream AgentDojo's task suites (most of these fixes have been merged upstream). It also removes certain tasks that are of low quality.\n\n3. It adds new injection tasks in the Workspace environment that have to do with mass data exfiltration (these have since been merged upstream).\n\n4. It adds a new terminal environment and associated tasks that test for remote code execution vulnerabilities in this environment.\n\n[1] Greshake K, Abdelnabi S, Mishra S, Endres C, Holz T, Fritz M (2023) Not what you?ve signed up for: Compromising Real-World LLM-Integrated Applications with Indirect Prompt Injection (arXiv), arXiv:2302.12173. https://doi.org/10.48550/arXiv.2302.12173\n\n[2] Edoardo Debenedetti (2025) ethz-spylab/agentdojo. Available at https://github.com/ethz-spylab/agentdojo.\n\n[3] Debenedetti E, Zhang J, Balunovi? M, Beurer-Kellner L, Fischer M, Tram\u00e8r F (2024) AgentDojo: A Dynamic Environment to Evaluate Prompt Injection Attacks and Defenses for LLM Agents (arXiv), arXiv:2406.13352. https://doi.org/10.48550/arXiv.2406.13352\n\n[4] UK AI Safety Institute (2024) Inspect AI: Framework for Large Language Model\u00a0Evaluations. 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Trustworthy AI is: valid and reliable, safe, secure and resilient, accountable and transparent, explainable and interpretable, privacy-enhanced, and fair - with harmful bias managed1. Dioptra supports the Measure function of the NIST AI Risk Management Framework by providing functionality to assess, analyze, and track identified AI risks.\n\nDioptra provides a REST API, which can be controlled via an intuitive web interface, a Python client, or any REST client library of the user's choice for designing, managing, executing, and tracking experiments. 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This dataset was generated by TechSolve Inc. (techsolve.org) as a collaborative effort with NIST. Respondents were asked to observe and evaluate a machining process in which a rotary bit (the \"tool\") removed layers of a workpiece until the tool was worn to exhaustion. One trial and 19 official experiments were completed, one for each of 20 tools. Respondents were tasked with completing a survey in which they recorded their measurements of tool flank wear along all four tool chamfers, recorded their description of the cut in natural language, and rated the process and tool condition on a Likert scale, along with other measurements.","distribution_titles":["README","README","cleaned/dataset","cleaned/dataset","cleaned/dataset","cleaned/schema","prepared/dataset","prepared/dataset","prepared/dataset","prepared/schema","raw/dataset","raw/dataset","raw/dataset","raw/original"],"harvest_record":"https://catalog.data.gov/harvest_record/ad3fb85f-5c18-4dc1-9a58-f793e7143be7","harvest_record_raw":"https://catalog.data.gov/harvest_record/ad3fb85f-5c18-4dc1-9a58-f793e7143be7/raw","has_download":true,"has_spatial":false,"identifier":"ark:/88434/mds2-3247","keyword":["image and signal processing","language processing","machining","manufacturing","natural language processing","process measurement and control","technical language processing","text"],"last_harvested_date":"2026-09-02T19:18:57.082480","organization":{"aliases":[""],"code_repo_exempt":false,"code_repo_url":null,"description":null,"id":"176f2a2d-ca9b-41f2-8df3-d93096ebdb85","logo":"https://raw.githubusercontent.com/GSA/logo/refs/heads/master/nist.png","name":"National Institute of Standards and Technology","organization_type":"Federal Government","slug":"nist"},"parent_identifier":null,"popularity":0,"publisher":"National Institute of Standards and Technology","slug":"human-observational-data-in-a-production-environment","spatial_centroid":null,"spatial_shape":null,"theme":["Manufacturing:Factory communications","Manufacturing:Factory operations planning and control","Manufacturing:Machining","Manufacturing:Manufacturing systems design and analysis","Manufacturing:Process improvement","Manufacturing:Process measurement and control","Mathematics and Statistics:Image and signal processing"],"title":"Human Observational Data in a Production Environment","type":"dataset"},{"_score":15.017646,"_sort":[1788376734532,15.017646,2,"9cd8e22b-3696-4ea9-9570-1af00957b759"],"dcat":{"@type":"dcat:Dataset","accessLevel":"public","accrualPeriodicity":"irregular","bureauCode":["006:55"],"contactPoint":{"fn":"Anna Karion","hasEmail":"mailto:anna.karion@nist.gov"},"description":"Methane (CH4) mole fraction data collected from three tower sites in the Washington DC area: Bucktown, MD (BUC, ghg01), Stafford, VA (SFD, ghg65), and Thurmont, MD (TMD, ghg61), as part \nof NIST's Northeast Corridor Urban Testbed project, presented as 1-minute averages.  This data is published for research academic and related non-commercial purposes consistent with NIST?s mandate to further the science and the promulgation of appropriate standards. \n\nThis dataset was used in the following publication and this archive represents the static archive of the data used in the publication and is not updated or modified: \n \nSahu, S., Ahn, D., Loughner, C., and Dickerson, R., \"Influence of synoptic weather patterns on methane mixing ratios in the Baltimore/Washington region\", Atmospheric Environment, Volume 334, 2024, 120675, ISSN 1352-2310,\nhttps://doi.org/10.1016/j.atmosenv.2024.120675.\n\nData is described further in the Readme document and references cited 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gas measurements","Methane","Washington DC","northeast corridor","urban testbed"],"landingPage":"https://data.nist.gov/od/id/mds2-3200","language":["en"],"license":"https://www.nist.gov/open/license","modified":"2024-03-18 00:00:00","programCode":["006:047"],"publisher":{"@type":"org:Organization","name":"National Institute of Standards and Technology"},"references":["https://doi.org/10.1016/j.atmosenv.2024.120675","https://doi.org/10.5194/essd-12-699-2020"],"rights":"Non-commercial use only.","temporal":"2015-01-01/2022-12-31","theme":["Environment:Greenhouse gas measurements"],"title":"In situ methane mole fraction observations from three sites in the Washington DC region from the NIST Northeast Corridor Project: January 2015 - December 2022"},"description":"Methane (CH4) mole fraction data collected from three tower sites in the Washington DC area: Bucktown, MD (BUC, ghg01), Stafford, VA (SFD, ghg65), and Thurmont, MD (TMD, ghg61), as part \nof NIST's Northeast Corridor Urban Testbed project, presented as 1-minute averages.  This data is published for research academic and related non-commercial purposes consistent with NIST?s mandate to further the science and the promulgation of appropriate standards. \n\nThis dataset was used in the following publication and this archive represents the static archive of the data used in the publication and is not updated or modified: \n \nSahu, S., Ahn, D., Loughner, C., and Dickerson, R., \"Influence of synoptic weather patterns on methane mixing ratios in the Baltimore/Washington region\", Atmospheric Environment, Volume 334, 2024, 120675, ISSN 1352-2310,\nhttps://doi.org/10.1016/j.atmosenv.2024.120675.\n\nData is described further in the Readme document and references cited within.\n","distribution_titles":[],"harvest_record":"https://catalog.data.gov/harvest_record/a834fc0e-0589-4685-b89a-6125ced4b1f4","harvest_record_raw":"https://catalog.data.gov/harvest_record/a834fc0e-0589-4685-b89a-6125ced4b1f4/raw","has_download":true,"has_spatial":false,"identifier":"ark:/88434/mds2-3200","keyword":["Bucktown","Greenhouse gas measurements","Methane","Washington DC","northeast corridor","urban testbed"],"last_harvested_date":"2026-09-02T19:18:54.532225","organization":{"aliases":[""],"code_repo_exempt":false,"code_repo_url":null,"description":null,"id":"176f2a2d-ca9b-41f2-8df3-d93096ebdb85","logo":"https://raw.githubusercontent.com/GSA/logo/refs/heads/master/nist.png","name":"National Institute of Standards and Technology","organization_type":"Federal Government","slug":"nist"},"parent_identifier":null,"popularity":2,"publisher":"National Institute of Standards and Technology","slug":"in-situ-methane-mole-fraction-observations-from-three-sites-in-the-washington-dc-regi-2022","spatial_centroid":null,"spatial_shape":null,"theme":["Environment:Greenhouse gas measurements"],"title":"In situ methane mole fraction observations from three sites in the Washington DC region from the NIST Northeast Corridor Project: January 2015 - December 2022","type":"dataset"},{"_score":27.868404,"_sort":[1788376731389,27.868404,2,"bc5de985-89d5-4fa6-8e85-0457e84284ef"],"dcat":{"@type":"dcat:Dataset","accessLevel":"public","accrualPeriodicity":"irregular","bureauCode":["006:55"],"contactPoint":{"fn":"Alain Rufenacht","hasEmail":"mailto:alain.rufenacht@nist.gov"},"description":"The abstract of the paper [1] is:\n\nThis paper describes differential sampling measurements of an ac source and a Josephson arbitrary waveform synthesizer (JAWS).\nA new iterative approach for aligning the phases of the JAWS and the source waveforms was implemented to minimize \nthe differential voltage at the digitizer. A type-A uncertainty of 45 nV/V after 10 min was measured for a commercial \nac source at 1 V rms amplitude and 1 kHz.\n\n[1] \"Differential Measurements of an AC Source with a Josephson Arbitrary Waveform Synthesizer\"submitted to Conference on Precision Electromagnetic Measurements (CPEM) 2024; will be published and available on IEEE website at a later date.\n\nData for figures 2 to 4 of the manuscript.\nFiles included in this publication:\n\n   Fig 2 FFT of the digitizer signal.csv\n\n    Figure 2\n    Fig. 2. 1 kHz component of the FFT of the digitizer signal (amplitude and phase) for Delta_V1=Source-JAWS1 and Delta_V2=Source-JAWS2 over 3.5 hours\n    Five columns: The first column is the time (x-axis), the second column is the amplitude in volt of the first measured difference voltage (shown as black solid circle in Fig. 2), \n    the third column is the phase in degree of the first measured difference voltage (shown as black open circle in Fig. 2),\n    the fourth column is the amplitude in volt of the second measured difference voltage (shown as red solid circle in Fig. 2),\n    the fifth column is the phase in degree of the second measured difference voltage (shown as red open circle in Fig. 2).\n    Format: CSV\n\n  Fig 3 Source rms amplitude and environment data.csv\n\n    Figure 3\n    Fig. 3. Room environment conditions recorded (temperature, atmospheric pressure, and relative humidity) and Reconstructed rms amplitude for the source at 1 kHz.\n    Five columns: The first column is the time (x-axis), the second column is the reconstructed amplitude in volt - 1 V (shown as blue solid circle in Fig. 3 bottom), \n    the third column is the temperature in degree C (shown as orange solid square in Fig. 3 top),\n    the fourth column is the atomsepheric pressure in hecto Pascal  (shown as green open triangle in Fig. 3 top),\n    the fifth column is the relative humidity in percent (shown as puple open circle in Fig. 2).\n    Format: CSV\n\n  Fig 4 Allan variance.csv\n\n    Figure 4\n    Fig. 4. Allan deviation of the source amplitude measured at 1 V and 1 kHz.\n    Five columns: The first column is the time (x-axis), the second column is the calculated Allan Deviation in volt (shown as blue solid circle in Fig. 4), \n    the third column is the fit on the results, representing the white noise with slope -0.5 (shown as black dash line in Fig. 4),\n    the fourth column is the is the time (x-axis) for the 1/f noise floor plot and the fifth column is the 1/f noise floor (shown as a black solid line in Fig. 4)\n    Format: CSV","distribution":[{"downloadURL":"https://data.nist.gov/od/ds/mds2-3162/3162_README.txt","mediaType":"text/plain","title":"3162_README"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3162/Fig%202%20FFT%20of%20the%20digitizer%20signal.csv","mediaType":"text/csv","title":"Fig 2 FFT of the digitizer signal"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3162/Fig%203%20Source%20rms%20amplitude%20and%20environment%20data.csv","mediaType":"text/csv","title":"Fig 3 Source rms amplitude and environment data"},{"downloadURL":"https://data.nist.gov/od/ds/mds2-3162/Fig%204%20Allan%20variance.csv","mediaType":"text/csv","title":"Fig 4 Allan variance"}],"identifier":"ark:/88434/mds2-3162","issued":"2024-02-13","keyword":["Josephson arrays","Measurement techniques","Standards","Superconducting integrated circuits","Voltage measurement"],"landingPage":"https://data.nist.gov/od/id/mds2-3162","language":["en"],"license":"https://www.nist.gov/open/license","modified":"2024-01-05 00:00:00","programCode":["006:045"],"publisher":{"@type":"org:Organization","name":"National Institute of Standards and Technology"},"theme":["Metrology:Electrical/electromagnetic metrology"],"title":"Differential Measurements of an AC Source with a Josephson Arbitrary Waveform Synthesizer"},"description":"The abstract of the paper [1] is:\n\nThis paper describes differential sampling measurements of an ac source and a Josephson arbitrary waveform synthesizer (JAWS).\nA new iterative approach for aligning the phases of the JAWS and the source waveforms was implemented to minimize \nthe differential voltage at the digitizer. A type-A uncertainty of 45 nV/V after 10 min was measured for a commercial \nac source at 1 V rms amplitude and 1 kHz.\n\n[1] \"Differential Measurements of an AC Source with a Josephson Arbitrary Waveform Synthesizer\"submitted to Conference on Precision Electromagnetic Measurements (CPEM) 2024; will be published and available on IEEE website at a later date.\n\nData for figures 2 to 4 of the manuscript.\nFiles included in this publication:\n\n   Fig 2 FFT of the digitizer signal.csv\n\n    Figure 2\n    Fig. 2. 1 kHz component of the FFT of the digitizer signal (amplitude and phase) for Delta_V1=Source-JAWS1 and Delta_V2=Source-JAWS2 over 3.5 hours\n    Five columns: The first column is the time (x-axis), the second column is the amplitude in volt of the first measured difference voltage (shown as black solid circle in Fig. 2), \n    the third column is the phase in degree of the first measured difference voltage (shown as black open circle in Fig. 2),\n    the fourth column is the amplitude in volt of the second measured difference voltage (shown as red solid circle in Fig. 2),\n    the fifth column is the phase in degree of the second measured difference voltage (shown as red open circle in Fig. 2).\n    Format: CSV\n\n  Fig 3 Source rms amplitude and environment data.csv\n\n    Figure 3\n    Fig. 3. Room environment conditions recorded (temperature, atmospheric pressure, and relative humidity) and Reconstructed rms amplitude for the source at 1 kHz.\n    Five columns: The first column is the time (x-axis), the second column is the reconstructed amplitude in volt - 1 V (shown as blue solid circle in Fig. 3 bottom), \n    the third column is the temperature in degree C (shown as orange solid square in Fig. 3 top),\n    the fourth column is the atomsepheric pressure in hecto Pascal  (shown as green open triangle in Fig. 3 top),\n    the fifth column is the relative humidity in percent (shown as puple open circle in Fig. 2).\n    Format: CSV\n\n  Fig 4 Allan variance.csv\n\n    Figure 4\n    Fig. 4. Allan deviation of the source amplitude measured at 1 V and 1 kHz.\n    Five columns: The first column is the time (x-axis), the second column is the calculated Allan Deviation in volt (shown as blue solid circle in Fig. 4), \n    the third column is the fit on the results, representing the white noise with slope -0.5 (shown as black dash line in Fig. 4),\n    the fourth column is the is the time (x-axis) for the 1/f noise floor plot and the fifth column is the 1/f noise floor (shown as a black solid line in Fig. 4)\n    Format: CSV","distribution_titles":["3162_README","Fig 2 FFT of the digitizer signal","Fig 3 Source rms amplitude and environment data","Fig 4 Allan variance"],"harvest_record":"https://catalog.data.gov/harvest_record/a388c5d5-7c17-4570-b60d-fa62500da89c","harvest_record_raw":"https://catalog.data.gov/harvest_record/a388c5d5-7c17-4570-b60d-fa62500da89c/raw","has_download":true,"has_spatial":false,"identifier":"ark:/88434/mds2-3162","keyword":["Josephson arrays","Measurement techniques","Standards","Superconducting integrated circuits","Voltage measurement"],"last_harvested_date":"2026-09-02T19:18:51.389318","organization":{"aliases":[""],"code_repo_exempt":false,"code_repo_url":null,"description":null,"id":"176f2a2d-ca9b-41f2-8df3-d93096ebdb85","logo":"https://raw.githubusercontent.com/GSA/logo/refs/heads/master/nist.png","name":"National Institute of Standards and Technology","organization_type":"Federal Government","slug":"nist"},"parent_identifier":null,"popularity":2,"publisher":"National Institute of Standards and Technology","slug":"differential-measurements-of-an-ac-source-with-a-josephson-arbitrary-waveform-synthesizer","spatial_centroid":null,"spatial_shape":null,"theme":["Metrology:Electrical/electromagnetic metrology"],"title":"Differential Measurements of an AC Source with a Josephson Arbitrary Waveform Synthesizer","type":"dataset"},{"_score":18.574387,"_sort":[1788376724578,18.574387,1,"31e2c124-8e55-40e2-9979-6855ffe68e28"],"dcat":{"@type":"dcat:Dataset","accessLevel":"public","bureauCode":["006:55"],"contactPoint":{"fn":"Michael Paul Majurski","hasEmail":"mailto:michael.majurski@nist.gov"},"description":"Round rl-randomized-lavaworld-aug2023-train Train Dataset\n\nThis is the training data used to create and evaluate trojan detection software solutions. 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This data, generated at NIST, consists of Reinforcement Learning agents trained to navigate the Lavaworld Minigrid environment. A known percentage of these trained AI models have been poisoned with a known trigger which induces incorrect behavior. 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The role of dual phosphorylation was explored by comparing 0P-ERK2 with 2P-ERK2 (two phosphate groups added at T183 and Y185). Both 0P-ERK2 and 2P-ERK2 models were treated with the ff19SB forcefield immersed in a solution of 0.15 M NaCl in OPC water. The results showed that the A-loop can adopt multiple long-lived (>5 microseconds) conformational states. A set of primary and secondary seeds were used to explore these novel states of the activation loop. Analysis scripts, dataframes, and all trajectories (stripped of explicit water and NaCl ions) are provided here to enhance the reproducibility of this complex study and aid future studies.\n \nTrajectories\n \nAs described in the associated publication, individual trajectories were run for (5-25) microseconds and totaled 727 microseconds. Multiple primary seeds (285 K, 300 K, 315 K, and 330 K) and secondary trajectory seeds (300 K) were run; all are available in this data publication. All frames for each trajectory were aligned to backbone atoms of residues 10-161 and 182-343 of the minimized 2ERK X-ray structures (0P and 2P). Modeled residue numbers are 1-353 and correspond to residues 6-358 of 2ERK and 5UMO (rat sequence numbering). The model built from 2Y9Q, which is a human kinase, was converted to correspond to the rat-derived models (2ERK, 5UMO) as described in the associated publication. Most primary seeds are greater than 10 microseconds while most secondary seeds are 5.7 microseconds. Angstrom units (0.1 nm) are used for trajectory coordinate storage and analysis. Three sets of trajectories are provided for convenience:\n \n1. The canonical set of trajectories are netcdf files (extension .nc) that are stripped of NaCl and water molecules and down-sampled to 2.5 ns between frames.\n \n2. The set of trajectory seeds with hydrogens removed and further down-sampling to 250 ns between frames is provided as DCD trajectory files. This is the smallest download that will be most convenient for visualization and initial development.\n \n3. Frames from the 300 K trajectories collated by the A-loop states. These trajectories should be treated as collections of frames without regard for any time information stored.\n \nStructures from RCSB.org\n \nThe associated publication analyzed the crystal packing environment of the activation loop. The structural data were collected in November 2021. All pdb files downloaded at that time are included in this data publication to aid the reproducibility of the analysis. The RCSB (Research Collaboratory for Structural Bioinformatics, https://www.rcsb.org) was the source of information and should be used directly for current versions of the associated entries. The RCSB entries pdbid 2ERK, pdbid 5UMO, and pdbid 2Y9Q were the structures used to build initial models for MD simulations.\n \nScripts\n \nRepresentative scripts are provided to aid future work. 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Similar products by other developers may be found to work as well or 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All frames for each trajectory were aligned to backbone atoms of residues 10-161 and 182-343 of the minimized 2ERK X-ray structures (0P and 2P). Modeled residue numbers are 1-353 and correspond to residues 6-358 of 2ERK and 5UMO (rat sequence numbering). The model built from 2Y9Q, which is a human kinase, was converted to correspond to the rat-derived models (2ERK, 5UMO) as described in the associated publication. Most primary seeds are greater than 10 microseconds while most secondary seeds are 5.7 microseconds. Angstrom units (0.1 nm) are used for trajectory coordinate storage and analysis. Three sets of trajectories are provided for convenience:\n \n1. The canonical set of trajectories are netcdf files (extension .nc) that are stripped of NaCl and water molecules and down-sampled to 2.5 ns between frames.\n \n2. The set of trajectory seeds with hydrogens removed and further down-sampling to 250 ns between frames is provided as DCD trajectory files. This is the smallest download that will be most convenient for visualization and initial development.\n \n3. Frames from the 300 K trajectories collated by the A-loop states. These trajectories should be treated as collections of frames without regard for any time information stored.\n \nStructures from RCSB.org\n \nThe associated publication analyzed the crystal packing environment of the activation loop. The structural data were collected in November 2021. All pdb files downloaded at that time are included in this data publication to aid the reproducibility of the analysis. The RCSB (Research Collaboratory for Structural Bioinformatics, https://www.rcsb.org) was the source of information and should be used directly for current versions of the associated entries. The RCSB entries pdbid 2ERK, pdbid 5UMO, and pdbid 2Y9Q were the structures used to build initial models for MD simulations.\n \nScripts\n \nRepresentative scripts are provided to aid future work. See README.md\n \nUnits\n \nQ-Aloop values are fractions. RMSD, distances, and coordinates are all reported in Angstroms (0.1 nm). Angles are reported in degrees.\n \nNOTE: Trade names are provided only to specify the source of information and procedures adequately and do not imply endorsement by the National Institute of Standards and Technology. 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