1
|
Bohon J, Gonzalez E, Grace C, Harris CT, Jacobsen B, Kachiguine S, Kim D, MacArthur J, Martinez-McKinney F, Mazza S, Nizam M, Norvell N, Padilla R, Potter E, Prakash T, Prebys E, Ryan E, Schumm BA, Smedley J, Stuart D, Tarka M, Torrecilla IS, Wilder M, Zhu D. Use of diamond sensors for a high-flux, high-rate X-ray pass-through diagnostic. J Synchrotron Radiat 2022; 29:595-601. [PMID: 35510992 PMCID: PMC9070720 DOI: 10.1107/s1600577522003022] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 12/18/2021] [Accepted: 03/19/2022] [Indexed: 06/14/2023]
Abstract
X-ray free-electron lasers (XFELs) deliver pulses of coherent X-rays on the femtosecond time scale, with potentially high repetition rates. While XFELs provide high peak intensities, both the intensity and the centroid of the beam fluctuate strongly on a pulse-to-pulse basis, motivating high-rate beam diagnostics that operate over a large dynamic range. The fast drift velocity, low X-ray absorption and high radiation tolerance properties of chemical vapour deposition diamonds make these crystals a promising candidate material for developing a fast (multi-GHz) pass-through diagnostic for the next generation of XFELs. A new approach to the design of a diamond sensor signal path is presented, along with associated characterization studies performed in the XPP endstation of the LINAC Coherent Light Source (LCLS) at SLAC. Qualitative charge collection profiles (collected charge versus time) are presented and compared with those from a commercially available detector. Quantitative results on the charge collection efficiency and signal collection times are presented over a range of approximately four orders of magnitude in the generated electron-hole plasma density.
Collapse
Affiliation(s)
- J. Bohon
- Los Alamos National Laboratory, Los Alamos, NM 87545, USA
| | - E. Gonzalez
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - C. Grace
- Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
| | - C. T. Harris
- Sandia National Laboratories, Albuquerque, NM 87123, USA
| | - B. Jacobsen
- SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - S. Kachiguine
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - D. Kim
- Los Alamos National Laboratory, Los Alamos, NM 87545, USA
| | - J. MacArthur
- SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - F. Martinez-McKinney
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - S. Mazza
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - M. Nizam
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - N. Norvell
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - R. Padilla
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - E. Potter
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - T. Prakash
- Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
| | - E. Prebys
- University of California, Davis, CA 95616, USA
| | - E. Ryan
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - B. A. Schumm
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - J. Smedley
- Los Alamos National Laboratory, Los Alamos, NM 87545, USA
| | - D. Stuart
- University of California, Santa Barbara, CA 93106, USA
| | - M. Tarka
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | | | - M. Wilder
- Santa Cruz Institute for Particle Physics, University of California, Santa Cruz, CA 95064, USA
| | - D. Zhu
- SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| |
Collapse
|
2
|
Hottowy P, Skoczeń A, Gunning DE, Kachiguine S, Mathieson K, Sher A, Wiącek P, Litke AM, Dąbrowski W. Properties and application of a multichannel integrated circuit for low-artifact, patterned electrical stimulation of neural tissue. J Neural Eng 2012; 9:066005. [PMID: 23160018 DOI: 10.1088/1741-2560/9/6/066005] [Citation(s) in RCA: 37] [Impact Index Per Article: 3.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/11/2022]
Abstract
OBJECTIVE Modern multielectrode array (MEA) systems can record the neuronal activity from thousands of electrodes, but their ability to provide spatio-temporal patterns of electrical stimulation is very limited. Furthermore, the stimulus-related artifacts significantly limit the ability to record the neuronal responses to the stimulation. To address these issues, we designed a multichannel integrated circuit for a patterned MEA-based electrical stimulation and evaluated its performance in experiments with isolated mouse and rat retina. APPROACH The Stimchip includes 64 independent stimulation channels. Each channel comprises an internal digital-to-analogue converter that can be configured as a current or voltage source. The shape of the stimulation waveform is defined independently for each channel by the real-time data stream. In addition, each channel is equipped with circuitry for reduction of the stimulus artifact. MAIN RESULTS Using a high-density MEA stimulation/recording system, we effectively stimulated individual retinal ganglion cells (RGCs) and recorded the neuronal responses with minimal distortion, even on the stimulating electrodes. We independently stimulated a population of RGCs in rat retina, and using a complex spatio-temporal pattern of electrical stimulation pulses, we replicated visually evoked spiking activity of a subset of these cells with high fidelity. Significance. Compared with current state-of-the-art MEA systems, the Stimchip is able to stimulate neuronal cells with much more complex sequences of electrical pulses and with significantly reduced artifacts. This opens up new possibilities for studies of neuronal responses to electrical stimulation, both in the context of neuroscience research and in the development of neuroprosthetic devices.
Collapse
Affiliation(s)
- Paweł Hottowy
- Faculty of Physics and Applied Computer Science, AGH University of Science and Technology, al. Mickiewicza 30, 30-059 Krakow, Poland.
| | | | | | | | | | | | | | | | | |
Collapse
|
3
|
Szuts TA, Fadeyev V, Kachiguine S, Sher A, Grivich MV, Agrochão M, Hottowy P, Dabrowski W, Lubenov EV, Siapas AG, Uchida N, Litke AM, Meister M. A wireless multi-channel neural amplifier for freely moving animals. Nat Neurosci 2011; 14:263-9. [DOI: 10.1038/nn.2730] [Citation(s) in RCA: 145] [Impact Index Per Article: 11.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/21/2010] [Accepted: 12/06/2010] [Indexed: 11/09/2022]
|