2021
DOI: 10.1109/tns.2020.3044489
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Development of a Tabletop Setup for the Transient Current Technique Using Two-Photon Absorption in Silicon Particle Detectors

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Cited by 16 publications
(18 citation statements)
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References 13 publications
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“…Good examples of such detectors are monolithic silicon pixel detectors [3,4], multipixel silicon LGAD detectors [5][6][7][8], detectors with 3D electrodes (silicon and diamond) [9,10], etc. Studying the charge transport in such structures is most frequently accomplished today by different variations of the TCT (transient current technique) technique, which uses laser light to create charge carriers in certain detector regions, generally through the small openings in electrodes that enable passage of light [11,12]. Other techniques are based on the induction of charge carriers from different radiation sources, such as electrons from accelerators, radioactive sources (e.g., betas from Sr90) or electron microscopy (SEM-EBIC) [13], focused X-rays from tube or synchrotron light, and finally a variety of heavier charge particles from radioisotope sources (e.g., alphas from Am241) or accelerators (IBIC) [14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…Good examples of such detectors are monolithic silicon pixel detectors [3,4], multipixel silicon LGAD detectors [5][6][7][8], detectors with 3D electrodes (silicon and diamond) [9,10], etc. Studying the charge transport in such structures is most frequently accomplished today by different variations of the TCT (transient current technique) technique, which uses laser light to create charge carriers in certain detector regions, generally through the small openings in electrodes that enable passage of light [11,12]. Other techniques are based on the induction of charge carriers from different radiation sources, such as electrons from accelerators, radioactive sources (e.g., betas from Sr90) or electron microscopy (SEM-EBIC) [13], focused X-rays from tube or synchrotron light, and finally a variety of heavier charge particles from radioisotope sources (e.g., alphas from Am241) or accelerators (IBIC) [14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…We have presented pulse durations as short as 13.0 fs (3.7 cycles), with a central wavelength of 1060 nm, but this is a non-fundamental limit that we expect to overcome with enhanced bre manufacture precision to obtain atter and nearer to zero dispersion curves of the ANDi PCFs. Based on the all-bre con guration reported here, our future work aims at increasing the output average power to the few-watts level (by increasing the pulse repetition rate of the bre oscillator seed to the GHz range 48 ) and at obtaining few-cycle emission at central wavelengths of 1.5 mm and 2.0 mm, particularly useful for localized nonlinear excitation of semiconductor materials transparent to these wavelengths 49 .…”
Section: Discussionmentioning
confidence: 99%
“…The multiphoton process requires a high density of photons to achieve a significant probability of multiple photons interacting simultaneously. As described in [5], the optical absorption in silicon is given by:…”
Section: Two-photon Absorption Laser Systemmentioning
confidence: 99%
“…These points deviate from the expected curve, however an explanation for this behaviour is not yet found. The voxel becomes effectively longer in silicon due to the change in refractive index at the air-silicon interface, as described in [5]. Therefore, the effective position 𝑧 within the silicon is given by…”
Section: Two-photon Absorption Laser Systemmentioning
confidence: 99%
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