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That is, we only compute fluxes for frequencies within our pulse bandwidth.
This is important because, to far outside the pulse bandwidth, the spectral power is so low that numerical errors make the computed fluxes useless.
In collaboration with students and colleagues at MIT, Goyal has achieved speed-ups in MRI, explained logarithmic scaling in human perception, and realized unprecedented resolution relative to pulse bandwidth and detector sampling rate in an active optical ranging.
Moreover, the optimization of the spoke placement is repeated with an increased pulse bandwidth in order to investigate the impact of the constraints on the result.
The carrier frequency, the pulse bandwidth, and PRF are f c = 1 GHz, B = 10 MHz, and f r = 2kHz, respectively.
To do so, we would need a minimum subcarrier spacing of equal to twice the one-sided pulse bandwidth, leading to F0=(1+?)R.
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These artifacts are exacerbated at high magnetic field due to the increased frequency dispersion, coupled with the limited RF pulse bandwidths used for localization.
The carrier frequency, sub-pulses bandwidth, and the PRF are respectively f c = 1 GHz, B = 10 MHz, and f r = 2 kHz.
With frequency-swept pulses, bandwidths of up to 800 MHz have previously been attained for excitation and detection of spin packets at frequencies of about 9.6 GHz and bandwidths of up to 2.5 GHz in a polarization transfer experiment at frequencies of about 34 GHz.
Band-selective inversion pulses are characterized by almost rectangular inversion profiles, leading to full inversion for spin packets with resonance offsets within the pulse excitation bandwidth and leaving spin packets outside the excitation bandwidth largely unaffected.
As the pulse length bandwidth product increases, the exact function tends to that of the wideband ideal system for which T1=T/2 and T2 = T/√(12), T being the transmitter pulse length.
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