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/content/aip/journal/rsi/87/11/10.1063/1.4962246
1.
R. J. Smith, Rev. Sci. Instrum. 79(10), 10E703 (2008).
http://dx.doi.org/10.1063/1.2981169
2.
A. J. Rogers, Appl. Opt. 20(6), 10601074 (1981).
http://dx.doi.org/10.1364/AO.20.001060
3.
A. V. Smith, B. T. Do, G. R. Hadley, and R. L. Farrow, IEEE J. Sel. Top. Quantum Electron. 15(1), 153158 (2009).
http://dx.doi.org/10.1109/JSTQE.2008.2010331
4.
M. Han, Y. Wang, and A. Wang, Opt. Lett. 32(14), 20282030 (2007).
http://dx.doi.org/10.1364/OL.32.002028
5.
K. H. Burrell, T. E. Evans, E. J. Doyle, M. E. Fenstermacher, R. J. Groebner, A. W. Leonard, R. A. Moyer, T. H. Osborne, M. J. Schaffer, P. B. Snyder et al., Plasma Phys. Controlled Fusion 47(12B), B37 (2005).
http://dx.doi.org/10.1088/0741-3335/47/12B/S04
6.
C. B. Forest, K. Flanagan, M. Brookhart, M. Clark, C. M. Cooper, V. Désangles, J. Egedal, D. Endrizzi, I. V. Khalzov, H. Li et al., J. Plasma Phys. 81(05), 345810501 (2015).
http://dx.doi.org/10.1017/S0022377815000975
7.
M. J. Rosenberg, C. K. Li, W. Fox, I. Igumenshchev, F. H. Séguin, R. P. J. Town, J. A. Frenje, C. Stoeckl, V. Glebov, and R. D. Petrasso, Nat. Commun. 6, 6190 (2015).
http://dx.doi.org/10.1038/ncomms7190
8.
G. Fiksel, W. Fox, A. Bhattacharjee, D. H. Barnak, P.-Y Chang, K. Germaschewski, S. X. Hu, and P. M. Nilson, Phys. Rev. Lett. 113(10), 105003 (2014).
http://dx.doi.org/10.1103/PhysRevLett.113.105003
9.
D. H. Goldstein, Polarized Light (CRC press, 2010).
http://aip.metastore.ingenta.com/content/aip/journal/rsi/87/11/10.1063/1.4962246
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/content/aip/journal/rsi/87/11/10.1063/1.4962246
2016-09-02
2016-09-30

Abstract

The technique of fiber optic pulsed polarimetry, which provides a distributed () measurement of the magnetic field along an optical fiber, has been improved to the point where, for the first time, photocathode based optical detection of backscatter is possible with sub-mm spatial resolutions. This has been realized through the writing of an array of deterministic fiber Bragg gratings along the fiber, a so-called - optical fiber, producing a 34 000-fold increase in backscatter levels over Rayleigh. With such high backscatter levels, high repetition rate lasers are now sufficiently bright to allow near continuous field sensing in both space and time with field resolutions as low as 0.005 T and as high as 170 T over a ∼mm interval given available fiber materials.

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