1969
DOI: 10.1016/0029-554x(69)90205-5
|View full text |Cite
|
Sign up to set email alerts
|

The Fourier method in slow neutron time-of-flight spectrometry

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
6
0

Year Published

1969
1969
2016
2016

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 20 publications
(6 citation statements)
references
References 2 publications
0
6
0
Order By: Relevance
“…It may be the correlation spectroscopy with pseudo-random flux modulation [25][26][27][28][29][30][31][32][33] or Fourier spectroscopy with periodic or quasiperiodic flux modulation [34][35][36][37][38][39][40][41][42].…”
Section: Introductionmentioning
confidence: 99%
“…It may be the correlation spectroscopy with pseudo-random flux modulation [25][26][27][28][29][30][31][32][33] or Fourier spectroscopy with periodic or quasiperiodic flux modulation [34][35][36][37][38][39][40][41][42].…”
Section: Introductionmentioning
confidence: 99%
“…In the pseudo-random method, the beam intensity is modulated with a periodic binary pseudo-random signal (figure 1(A)) and the time-of-flight spectrum is calculated as the cross-correlation of the modulation signal and the detector output [2]. The Fourier diffractometer involves modulation of the neutron beam by a fast Fourier chopper [3] (figure 1(B)) which is a rotating disc (rotor) with a pattern of alternating neutron absorbing and neutron transparent slits; and a fixed system of identical slits (stator). The method consists of measuring the Fourier transform of the time-of-flight spectrum at several discrete frequencies and forming the spectrum itself by Fourier synthesis from the measured frequency components.…”
Section: Tof Methodsmentioning
confidence: 99%
“…[40][41][42] Alternatively, such sequences are referred to in literature as pseudonoise sequences or m-sequences. 40 Particular methods for generation of pseudorandom sequences 43,44 were developed in connection with communication and encryption processes, 45 acoustics, 46 and pseudorandom chopping of a beam in time-of-flight experiments with slow neutrons [47][48][49][50][51][52] and molecular beams. [53][54][55] The maximum duty cycle (relative number of 1's and 0's) of approximately 50% is obtained with a maximum-length pseudorandom sequence (MLPRS).…”
Section: Bpr Sequences and Arraysmentioning
confidence: 99%
“…URAs are widely used as optimal mask patterns for coded aperture imaging techniques. 41 Analogous to the time-of-flight technique based on 1D BPR sequence chopping, [47][48][49][50][51][52][53][54][55] an imaging technique based on the 2D URAs allows one to obtain a better signal-to-noise ratio, keeping the high angular resolution characteristic of a single pinhole aperture. [57][58][59] Similar to 1D BPR sequences, the URAs possess both high throughput (50%) and a delta-function-like cyclical autocorrelation function that corresponds to a flat 2D PSD spectrum.…”
Section: Bpr Sequences and Arraysmentioning
confidence: 99%