TY - JOUR
T1 - DAC-board based X-band EPR spectrometer with arbitrary waveform control
AU - Kaufmann, Thomas
AU - Keller, Timothy J.
AU - Franck, John M.
AU - Barnes, Ryan P.
AU - Glaser, Steffen J.
AU - Martinis, John M.
AU - Han, Songi
N1 - Funding Information:
We would like to express our sincere gratitude to Bruker BioSpin and especially Arthur Heiss, Charles Hanson, Ralph Weber, Peter Höfer, and Robert Dick for their dedicated and sustained support. We thank Steve Waltman (High Speed Circuit Consultants) for exceptional technical support and advice. We thank Daniel Sank, Dr. Yu Chen, Dr. Max Hofheinz, and Dr. Erik Lucero from the Martinis group for helpful advice pertaining to functioning of the DAC board. This work was funded by the National Science Foundation IDBR Grant, the National Institute of Health R21 Biomedical Instrument Development Grant, and the CNSI Elings Prize Postdoctoral Fellowship to J.M.F. S.J. Glaser acknowledges support from the DFG (Gl 203/7-1) and the Fonds der Chemischen Industrie.
PY - 2013
Y1 - 2013
N2 - We present arbitrary control over a homogenous spin system, demonstrated on a simple, home-built, electron paramagnetic resonance (EPR) spectrometer operating at 8-10 GHz (X-band) and controlled by a 1 GHz arbitrary waveform generator (AWG) with 42 dB (i.e. 14-bit) of dynamic range. Such a spectrometer can be relatively easily built from a single DAC (digital to analog converter) board with a modest number of stock components and offers powerful capabilities for automated digital calibration and correction routines that allow it to generate shaped X-band pulses with precise amplitude and phase control. It can precisely tailor the excitation profiles "seen" by the spins in the microwave resonator, based on feedback calibration with experimental input. We demonstrate the capability to generate a variety of pulse shapes, including rectangular, triangular, Gaussian, sinc, and adiabatic rapid passage waveforms. We then show how one can precisely compensate for the distortion and broadening caused by transmission into the microwave cavity in order to optimize corrected waveforms that are distinctly different from the initial, uncorrected waveforms. Specifically, we exploit a narrow EPR signal whose width is finer than the features of any distortions in order to map out the response to a short pulse, which, in turn, yields the precise transfer function of the spectrometer system. This transfer function is found to be consistent for all pulse shapes in the linear response regime. In addition to allowing precise waveform shaping capabilities, the spectrometer presented here offers complete digital control and calibration of the spectrometer that allows one to phase cycle the pulse phase with 0.007 resolution and to specify the inter-pulse delays and pulse durations to ≤250 ps resolution. The implications and potential applications of these capabilities will be discussed.
AB - We present arbitrary control over a homogenous spin system, demonstrated on a simple, home-built, electron paramagnetic resonance (EPR) spectrometer operating at 8-10 GHz (X-band) and controlled by a 1 GHz arbitrary waveform generator (AWG) with 42 dB (i.e. 14-bit) of dynamic range. Such a spectrometer can be relatively easily built from a single DAC (digital to analog converter) board with a modest number of stock components and offers powerful capabilities for automated digital calibration and correction routines that allow it to generate shaped X-band pulses with precise amplitude and phase control. It can precisely tailor the excitation profiles "seen" by the spins in the microwave resonator, based on feedback calibration with experimental input. We demonstrate the capability to generate a variety of pulse shapes, including rectangular, triangular, Gaussian, sinc, and adiabatic rapid passage waveforms. We then show how one can precisely compensate for the distortion and broadening caused by transmission into the microwave cavity in order to optimize corrected waveforms that are distinctly different from the initial, uncorrected waveforms. Specifically, we exploit a narrow EPR signal whose width is finer than the features of any distortions in order to map out the response to a short pulse, which, in turn, yields the precise transfer function of the spectrometer system. This transfer function is found to be consistent for all pulse shapes in the linear response regime. In addition to allowing precise waveform shaping capabilities, the spectrometer presented here offers complete digital control and calibration of the spectrometer that allows one to phase cycle the pulse phase with 0.007 resolution and to specify the inter-pulse delays and pulse durations to ≤250 ps resolution. The implications and potential applications of these capabilities will be discussed.
KW - Arbitrary waveform generation
KW - EPR
KW - Excitation profile
KW - Pulse electron paramagnetic resonance
KW - Transfer function
KW - X-band
UR - http://www.scopus.com/inward/record.url?scp=84883144415&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84883144415&partnerID=8YFLogxK
U2 - 10.1016/j.jmr.2013.07.015
DO - 10.1016/j.jmr.2013.07.015
M3 - Article
C2 - 23999530
AN - SCOPUS:84883144415
SN - 1090-7807
VL - 235
SP - 95
EP - 108
JO - Journal of Magnetic Resonance
JF - Journal of Magnetic Resonance
ER -