002875153 001__ 2875153
002875153 005__ 20240410042717.0
002875153 0248_ $$aoai:cds.cern.ch:2875153$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002875153 0247_ $$2DOI$$9IOP$$a10.1088/1748-0221/18/01/C01023$$qpublication
002875153 037__ $$9arXiv$$aarXiv:2210.13713$$cphysics.ins-det
002875153 035__ $$9arXiv$$aoai:arXiv.org:2210.13713
002875153 035__ $$9Inspire$$aoai:inspirehep.net:2170638$$d2024-04-09T13:06:11Z$$h2024-04-10T02:00:06Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002875153 035__ $$9Inspire$$a2170638
002875153 041__ $$aeng
002875153 100__ $$aNomerotski, [email protected]$$uBrookhaven$$vPhysics Department, Brookhaven National Laboratory, Upton NY 11973, U.S.A.
002875153 245__ $$9IOP$$aIntensified Tpx3Cam, a fast data-driven optical camera with nanosecond timing resolution for single photon detection in quantum applications
002875153 260__ $$c2023-01-17
002875153 269__ $$c2022-10-24
002875153 300__ $$a13 p
002875153 520__ $$9IOP$$aWe describe a fast data-driven optical camera, Tpx3Cam, with nanosecond scale timing resolution and 80 Mpixel/sec throughput. After the addition of intensifier, the camera is single photon sensitive with quantum efficiency determined primarily by the intensifier photocathode. The single photon performance of the camera was characterized with results on the gain, timing resolution and afterpulsing reported here. The intensified camera was successfully used for measurements in a variety of applications including quantum applications. As an example of such application, which requires simultaneous detection of multiple photons, we describe registration of photon pairs from the spontaneous parametric down-conversion source in a spectrometer. We measured the photon wavelength and timing with respective precisions of 0.15 nm and 3 ns, and also demonstrated that the two photons are anti-correlated in energy.
002875153 520__ $$9arXiv$$aWe describe a fast data-driven optical camera, Tpx3Cam, with nanosecond scale timing resolution and 80 Mpixel/sec throughput. After the addition of intensifier, the camera is single photon sensitive with quantum efficiency determined primarily by the intensifier photocathode. The single photon performance of the camera was characterized with results on the gain, timing resolution and afterpulsing reported here. The intensified camera was successfully used for measurements in a variety of applications including quantum applications. As an example of such application, which requires simultaneous detection of multiple photons, we describe registration of photon pairs from the spontaneous parametric down-conversion source in a spectrometer. We measured the photon wavelength and timing with respective precisions of 0.15~nm and 3~ns, and also demonstrated that the two photons are anti-correlated in energy.
002875153 541__ $$adesy$$chepcrawl$$d2023-01-19T16:01:43.996869$$e5062250
002875153 540__ $$3preprint$$aCC BY 4.0$$uhttp://creativecommons.org/licenses/by/4.0/
002875153 542__ $$3publication$$dIOP Publishing Ltd and Sissa Medialab$$g2023
002875153 595__ $$cCDS
002875153 65017 $$2arXiv$$aquant-ph
002875153 65017 $$2SzGeCERN$$aGeneral Theoretical Physics
002875153 65017 $$2arXiv$$aphysics.ins-det
002875153 65017 $$2SzGeCERN$$aDetectors and Experimental Techniques
002875153 690C_ $$aCERN
002875153 690C_ $$aARTICLE
002875153 700__ $$aChekhlov, Matthew$$uBrookhaven$$vPhysics Department, Brookhaven National Laboratory, Upton NY 11973, U.S.A.
002875153 700__ $$aDolzhenko, Denis$$uBrookhaven$$vPhysics Department, Brookhaven National Laboratory, Upton NY 11973, U.S.A.
002875153 700__ $$aGlazenborg, Rene$$uPhotonis, Brive$$vPhotonis Netherlands BV, 9301 ZR Roden, The Netherlands
002875153 700__ $$aFarella, Brianna$$uBrookhaven$$vPhysics Department, Brookhaven National Laboratory, Upton NY 11973, U.S.A.
002875153 700__ $$aKeach, Michael$$uBrookhaven$$vPhysics Department, Brookhaven National Laboratory, Upton NY 11973, U.S.A.
002875153 700__ $$aMahon, Ryan$$uBrookhaven$$vPhysics Department, Brookhaven National Laboratory, Upton NY 11973, U.S.A.
002875153 700__ $$aOrlov, Dmitry$$uPhotonis, Brive$$vPhotonis Netherlands BV, 9301 ZR Roden, The Netherlands
002875153 700__ $$aSvihra, Peter$$uPrague, Tech. U.$$uCERN$$vFaculty of Nuclear Sciences and Physical Engineering, Czech Technical University, 115 19 Prague, Czech Republic$$vExperimental Physics Department, CERN, 1211 Geneva 23, Switzerland
002875153 773__ $$cC01023$$mpublication$$n01$$pJINST$$v18$$wC22-06-26.3$$y2023
002875153 8564_ $$82483676$$s14742$$uhttps://cds.cern.ch/record/2875153/files/Comparison_plot.png$$y00005 Left: Two instances of TOT correction for the same camera taken at different times; Right: Time difference distribution for a pair of simultaneous photons from SPDC source after the TOT correction.
002875153 8564_ $$82483677$$s30817$$uhttps://cds.cern.ch/record/2875153/files/dt_plot_final.png$$y00009 Left: Distribution of distances for two successive hits. Right: Distribution of time differences for two successive hits.
002875153 8564_ $$82483678$$s205905$$uhttps://cds.cern.ch/record/2875153/files/argonSpectrum.png$$y00011 Left: Two argon spectra for two beams derived from the same argon lamp. Right: Spectrometer linearity, scale and residuals.
002875153 8564_ $$82483679$$s670276$$uhttps://cds.cern.ch/record/2875153/files/SPDCspectrum.png$$y00014 Left: Three argon lines in spectrometer with increased magnification. Right: Signal (top stripe) and idler (bottom stripe) photons in the spectrometer.
002875153 8564_ $$82483680$$s16716$$uhttps://cds.cern.ch/record/2875153/files/2D_hist_dx1_dy1.png$$y00007 Left: Two mechanisms of afterpulsing due to the ion feedback and secondary electrons. Right: Spatial distribution of the afterpulses. The empty square $3\times3$ pixels in the middle is due to the requirement of the two hits to be separated by at least one pixel.
002875153 8564_ $$82483681$$s4233700$$uhttps://cds.cern.ch/record/2875153/files/2210.13713.pdf$$yFulltext
002875153 8564_ $$82483682$$s57180$$uhttps://cds.cern.ch/record/2875153/files/timing1.png$$y00006 Left: Two instances of TOT correction for the same camera taken at different times; Right: Time difference distribution for a pair of simultaneous photons from SPDC source after the TOT correction.
002875153 8564_ $$82483683$$s6654$$uhttps://cds.cern.ch/record/2875153/files/npixels.png$$y00004 Left: time-over-threshold (TOT) distribution. Right: distribution of number of pixels in cluster.
002875153 8564_ $$82483684$$s1207711$$uhttps://cds.cern.ch/record/2875153/files/DCR-at-diff-Biases.png$$y00010 Normalized 2D occupancy for the intensifier dark counts for the silicon bias voltage between 0V and 60V.
002875153 8564_ $$82483685$$s4001951$$uhttps://cds.cern.ch/record/2875153/files/tpx3camPhoto.png$$y00001 Left: Schematic layout of the intensified Tpx3Cam camera, not to scale. Right: photograph of the camera with Cricket$^{\rm{TM}}$.
002875153 8564_ $$82483686$$s18285$$uhttps://cds.cern.ch/record/2875153/files/wavelength_anticorrelation_histogram.png$$y00015 Left: Anti-correlation of photon wavelengths for the SPDC source. Right: Reconstructed wavelength of the pump photon using the wavelengths of the signal and idler photons, and argon spectrum calibration.
002875153 8564_ $$82483687$$s6353$$uhttps://cds.cern.ch/record/2875153/files/TOT.png$$y00003 Left: time-over-threshold (TOT) distribution. Right: distribution of number of pixels in cluster.
002875153 8564_ $$82483688$$s18343$$uhttps://cds.cern.ch/record/2875153/files/SPDC_projection_dt_dlambda.png$$y00016 Left: Anti-correlation of photon wavelengths for the SPDC source. Right: Reconstructed wavelength of the pump photon using the wavelengths of the signal and idler photons, and argon spectrum calibration.
002875153 8564_ $$82483689$$s48747$$uhttps://cds.cern.ch/record/2875153/files/TPX3Camera.png$$y00000 Left: Schematic layout of the intensified Tpx3Cam camera, not to scale. Right: photograph of the camera with Cricket$^{\rm{TM}}$.
002875153 8564_ $$82483690$$s164190$$uhttps://cds.cern.ch/record/2875153/files/Linearity4.png$$y00012 Left: Two argon spectra for two beams derived from the same argon lamp. Right: Spectrometer linearity, scale and residuals.
002875153 8564_ $$82483691$$s157597$$uhttps://cds.cern.ch/record/2875153/files/Peaks3.png$$y00013 Left: Three argon lines in spectrometer with increased magnification. Right: Signal (top stripe) and idler (bottom stripe) photons in the spectrometer.
002875153 8564_ $$82483692$$s12210$$uhttps://cds.cern.ch/record/2875153/files/20min_Coincidences-Ex3.png$$y00002 Raw TOT (left) and TOA (right) values in nanoseconds for pairs of single photon hits in Tpx3Cam.
002875153 8564_ $$82483693$$s47021$$uhttps://cds.cern.ch/record/2875153/files/dist_final_hist.png$$y00008 Left: Distribution of distances for two successive hits. Right: Distribution of time differences for two successive hits.
002875153 960__ $$a13
002875153 962__ $$b2812513$$kC01023$$nriva del garda20220626
002875153 980__ $$aConferencePaper
002875153 980__ $$aARTICLE