-
1
-
-
0035900398
-
-
S.A. Wolf et al., Science 294, 1488 (2001).
-
(2001)
Science
, vol.294
, pp. 1488
-
-
Wolf, S.A.1
-
3
-
-
0009906761
-
-
G. Schmidt, D. Ferrand, L.W. Molenkamp, A.T. Filip, and B.J. van Wees, Phys. Rev. B 62, R4790 (2000).
-
(2000)
Phys. Rev. B
, vol.62
, pp. R4790
-
-
Schmidt, G.1
Ferrand, D.2
Molenkamp, L.W.3
Filip, A.T.4
van Wees, B.J.5
-
4
-
-
85038906334
-
-
cond-mat/0206347 (unpublished)
-
G. Schmidt, C. Gould, P. Grabs, A.M. Lunde, G. Richter, A. Slobodskyy, and L.W. Molenkamp, cond-mat/0206347 (unpublished).
-
-
-
Schmidt, G.1
Gould, C.2
Grabs, P.3
Lunde, A.M.4
Richter, G.5
Slobodskyy, A.6
Molenkamp, L.W.7
-
5
-
-
85038903606
-
-
cond-mat/0201425 (unpublished)
-
Z.G. Yu and M.E. Flatté, cond-mat/0201425 (unpublished);
-
-
-
Yu, Z.G.1
Flatté, M.E.2
-
6
-
-
85038929125
-
-
cond-mat/0206321 (unpublished)
-
Z.G. Yu and M.E. Flatté, cond-mat/0206321 (unpublished).
-
-
-
Yu, Z.G.1
Flatté, M.E.2
-
7
-
-
85038925410
-
-
E. I. Rashba, cond-mat/0206129, Euro. Phys. J. B (to be published)
-
E. I. Rashba, cond-mat/0206129, Euro. Phys. J. B (to be published).
-
-
-
-
13
-
-
0035947250
-
-
V.P. LaBella et al., Science 292, 1518 (2001);
-
(2001)
Science
, vol.292
, pp. 1518
-
-
LaBella, V.P.1
-
14
-
-
0012499310
-
-
ScienceW.F. Egelhoff, Jr. et al., 296, 1195a (2002);
-
(2002)
Science
, vol.296
, pp. 1195a
-
-
Egelhoff, W.F.1
-
15
-
-
0012499310
-
-
ScienceV.P. LaBella et al., 296, 1195a (2002).
-
(2002)
Science
, vol.296
, pp. 1195a
-
-
LaBella, V.P.1
-
19
-
-
85038901907
-
-
cond-mat/0203261 (unpublished)
-
A.A. Kiselev and K.W. Kim, cond-mat/0203261 (unpublished).
-
-
-
Kiselev, A.A.1
Kim, K.W.2
-
21
-
-
0036538488
-
-
M. Governale, D. Boese, U. Zülicke, and C. Schroll, Phys. Rev. B 65, 140403 (2002);
-
(2002)
Phys. Rev. B
, vol.65
, pp. 140403
-
-
Governale, M.1
Boese, D.2
Zülicke, U.3
Schroll, C.4
-
26
-
-
85038943046
-
-
We point out that even in the case in which a single-input design is considered (e.g., by replacing the first beam splitter with a Y junction), the corresponding device can still be used as a spin polarizer and all the results derived here for the output spin polarization apply as well. In this case, however, the device is no longer equivalent to a PBS or a Controlled-NOT gate and for this reason we prefer the four terminal design
-
We point out that even in the case in which a single-input design is considered (e.g., by replacing the first beam splitter with a Y junction), the corresponding device can still be used as a spin polarizer and all the results derived here for the output spin polarization apply as well. In this case, however, the device is no longer equivalent to a PBS or a Controlled-NOT gate and for this reason we prefer the four terminal design.
-
-
-
-
27
-
-
85038903638
-
-
A Mach-Zehnder interferometer was also considered by Seelig and Büttiker Ref. 21, in the context of charge decoherence in a AB ring
-
A Mach-Zehnder interferometer was also considered by Seelig and Büttiker Ref. 21, in the context of charge decoherence in a AB ring.
-
-
-
-
32
-
-
85038926617
-
-
If we inject spins in input 1 instead of 0, the transformations are (Formula presented) (Formula presented)
-
If we inject spins in input 1 instead of 0, the transformations are (Formula presented) (Formula presented)
-
-
-
-
36
-
-
85038895380
-
-
cond-mat/0002209 (unpublished)
-
A. Bachtoldcond-mat/0002209 (unpublished).
-
-
-
Bachtold, A.1
-
39
-
-
85038892776
-
-
This is one of the main differences between our proposal and the one described in Ref. 13,. Since in that case the interferometer is not balanced the interference pattern, and hence the transmission coefficients, are both energy dependent
-
This is one of the main differences between our proposal and the one described in Ref. 13,. Since in that case the interferometer is not balanced the interference pattern, and hence the transmission coefficients, are both energy dependent.
-
-
-
|