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1
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34548622598
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NATUAS 0028-0836 10.1038/nature06094
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D. B. Cassidy and A. P. Mills, Jr., Nature (London) NATUAS 0028-0836 10.1038/nature06094 449, 195 (2007).
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(2007)
Nature (London)
, vol.449
, pp. 195
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Cassidy, D.B.1
Mills Jr., A.P.2
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2
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0036576989
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NIMBEU 0168-583X 10.1016/S0168-583X(02)00790-5
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A. P. Mills, Jr., Nucl. Instrum. Methods Phys. Res. B NIMBEU 0168-583X 10.1016/S0168-583X(02)00790-5 192, 107 (2002).
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(2002)
Nucl. Instrum. Methods Phys. Res. B
, vol.192
, pp. 107
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Mills Jr., A.P.1
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3
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37649007867
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A. P. Mills, Jr., Appl. Surf. Sci. (to be published).
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Mills Jr., A.P.1
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4
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34548270920
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PRLTAO 0031-9007 10.1103/PhysRevLett.99.096101
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R. Saniz, B. Barbiellini, P. M. Platzman, and A. J. Freeman, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.99.096101 99, 096101 (2007).
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Phys. Rev. Lett.
, vol.99
, pp. 096101
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Saniz, R.1
Barbiellini, B.2
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Freeman, A.J.4
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5
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3142708481
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RMPHAT 0034-6861 10.1103/RevModPhys.60.701
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P. J. Schultz and K. G. Lynn, Rev. Mod. Phys. RMPHAT 0034-6861 10.1103/RevModPhys.60.701 60, 701 (1988).
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Rev. Mod. Phys.
, vol.60
, pp. 701
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Schultz, P.J.1
Lynn, K.G.2
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6
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4243870135
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Positron reemission is only possible if the material in question has a negative positron work function or the emitted positrons are not fully thermalized. PRLTAO 0031-9007 10.1103/PhysRevLett.41.1076
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Positron reemission is only possible if the material in question has a negative positron work function or the emitted positrons are not fully thermalized. A. P. Mills, Jr., P. M. Platzman, and B. L. Brown, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.41.1076 41, 1076 (1978).
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Phys. Rev. Lett.
, vol.41
, pp. 1076
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Mills Jr., A.P.1
Platzman, P.M.2
Brown, B.L.3
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7
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0015639249
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SSCOA4 0038-1098 10.1016/0038-1098(73)90133-6
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C. H. Hodges and M. J. Stott, Solid State Commun. SSCOA4 0038-1098 10.1016/0038-1098(73)90133-6 12, 1153 (1973).
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Hodges, C.H.1
Stott, M.J.2
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8
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4243639725
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PRLTAO 0031-9007 10.1103/PhysRevLett.33.7
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K. F. Canter, A. P. Mills, Jr., and S. Berko, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.33.7 33, 7 (1974).
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(1974)
Phys. Rev. Lett.
, vol.33
, pp. 7
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Canter, K.F.1
Mills Jr., A.P.2
Berko, S.3
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9
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0001273824
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See for example edited by A. Dupasquier and A. P. Mills, Jr. (IOS Press, Amsterdam
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See for example A. P. Mills, Jr., in Positron Spectroscopy of Solids, edited by, A. Dupasquier, and, A. P. Mills, Jr., (IOS Press, Amsterdam, 1995), pp. 209-258.
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(1995)
Positron Spectroscopy of Solids
, pp. 209-258
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Mills Jr., A.P.1
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10
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4043107996
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The neutral work function Ps = + + - has been introduced by PRLTAO 0031-9007 10.1103/PhysRevLett.60.1193
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The neutral work function Ps = + + - has been introduced by D. W. Gidley and W. E. Frieze, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.60.1193 60, 1193 (1988).
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(1988)
Phys. Rev. Lett.
, vol.60
, pp. 1193
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Gidley, D.W.1
Frieze, W.E.2
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11
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0542432469
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PRBMDO 0163-1829 10.1103/PhysRevB.33.5900
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P. M. Platzman and N. Tzoar, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.33.5900 33, 5900 (1986).
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(1986)
Phys. Rev. B
, vol.33
, pp. 5900
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Platzman, P.M.1
Tzoar, N.2
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12
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4143053655
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JPSOAW 0022-3719 10.1088/0022-3719/13/6/024
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J. B. Pendry, J. Phys. C JPSOAW 0022-3719 10.1088/0022-3719/13/6/024 13, 1159 (1980).
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(1980)
J. Phys. C
, vol.13
, pp. 1159
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Pendry, J.B.1
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13
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0009575123
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PRBMDO 0163-1829 10.1103/PhysRevB.23.2060
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S. Chu, A. P. Mills, Jr., and C. A. Murray, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.23.2060 23, 2060 (1981).
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(1981)
Phys. Rev. B
, vol.23
, pp. 2060
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Chu, S.1
Mills Jr., A.P.2
Murray, C.A.3
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14
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0001932493
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PRBMDO 0163-1829 10.1103/PhysRevB.32.53
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A. P. Mills, Jr. and L. Pfeiffer, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.32.53 32, 53 (1985).
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(1985)
Phys. Rev. B
, vol.32
, pp. 53
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Mills Jr., A.P.1
Pfeiffer, L.2
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15
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4243980785
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PRLTAO 0031-9007 10.1103/PhysRevLett.66.735
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A. P. Mills, Jr., E. D. Shaw, M. Leventhal, P. M. Platzman, R. J. Chichester, D. M. Zuckerman, T. Martin, R. Bruinsma, and R. R. Lee, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.66.735 66, 735 (1991).
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(1991)
Phys. Rev. Lett.
, vol.66
, pp. 735
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Mills Jr., A.P.1
Shaw, E.D.2
Leventhal, M.3
Platzman, P.M.4
Chichester, R.J.5
Zuckerman, D.M.6
Martin, T.7
Bruinsma, R.8
Lee, R.R.9
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16
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0001394790
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PLRAAN 1050-2947 10.1103/PhysRevA.58.1918
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J. Usukura, K. Varga, and Y. Suzuki, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.58.1918 58, 1918 (1998).
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(1998)
Phys. Rev. A
, vol.58
, pp. 1918
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Usukura, J.1
Varga, K.2
Suzuki, Y.3
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17
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0018517399
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SSCOA4 0038-1098 10.1016/0038-1098(79)90310-7
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A. P. Mills, Jr., Solid State Commun. SSCOA4 0038-1098 10.1016/0038-1098(79)90310-7 31, 623 (1979).
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(1979)
Solid State Commun.
, vol.31
, pp. 623
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Mills Jr., A.P.1
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18
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1442331419
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E.g., PRLTAO 0031-9007 10.1103/PhysRevLett.92.043401
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E.g., D. M. Schrader, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.92.043401 92, 043401 (2004);
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Phys. Rev. Lett.
, vol.92
, pp. 043401
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Schrader, D.M.1
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19
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33751119941
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PLRAAN 1050-2947 10.1103/PhysRevA.74.052502
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S. Bubin and L. Adamowicz, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.74.052502 74, 052502 (2006).
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(2006)
Phys. Rev. A
, vol.74
, pp. 052502
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Bubin, S.1
Adamowicz, L.2
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20
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33646680265
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APPLAB 0003-6951 10.1063/1.2203336
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D. B. Cassidy, S. H. M. Deng, H. K. M. Tanaka, and A. P. Mills, Jr., Appl. Phys. Lett. APPLAB 0003-6951 10.1063/1.2203336 88, 194105 (2006).
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(2006)
Appl. Phys. Lett.
, vol.88
, pp. 194105
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Cassidy, D.B.1
Deng, S.H.M.2
Tanaka, H.K.M.3
Mills Jr., A.P.4
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21
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33746834863
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RSINAK 0034-6748 10.1063/1.2221509
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D. B. Cassidy, S. H. M. Deng, R. G. Greaves, and A. P Mills, Jr., Rev. Sci. Instrum. RSINAK 0034-6748 10.1063/1.2221509 77, 073106 (2006).
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(2006)
Rev. Sci. Instrum.
, vol.77
, pp. 073106
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Cassidy, D.B.1
Deng, S.H.M.2
Greaves, R.G.3
P Mills Jr., A.4
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22
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2942573113
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PHPAEN 1070-664X 10.1063/1.1651487
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C. M. Surko and R. G. Greaves, Phys. Plasmas PHPAEN 1070-664X 10.1063/1.1651487 11, 2333 (2004).
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(2004)
Phys. Plasmas
, vol.11
, pp. 2333
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Surko, C.M.1
Greaves, R.G.2
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23
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0019033215
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APHYCC 0340-3793 10.1007/BF00899876
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A. P. Mills, Jr., Appl. Phys. (Berlin) APHYCC 0340-3793 10.1007/BF00899876 22, 273 (1980).
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(1980)
Appl. Phys. (Berlin)
, vol.22
, pp. 273
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Mills Jr., A.P.1
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25
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0034726308
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PRLTAO 0031-9007 10.1103/PhysRevLett.85.1883
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R. G. Greaves and C. M. Surko, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.85.1883 85, 1883 (2000).
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Phys. Rev. Lett.
, vol.85
, pp. 1883
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Greaves, R.G.1
Surko, C.M.2
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26
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35949021841
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RMPHAT 0034-6861 10.1103/RevModPhys.53.127
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A. Rich, Rev. Mod. Phys. RMPHAT 0034-6861 10.1103/RevModPhys.53.127 53, 127 (1981).
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(1981)
Rev. Mod. Phys.
, vol.53
, pp. 127
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Rich, A.1
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28
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28844475248
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PRLTAO 0031-9007 10.1103/PhysRevLett.95.195006
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D. B. Cassidy, S. H. M. Deng, R. G. Greaves, T. Maruo, N. Nishiyama, J. B. Snyder, H. K. M. Tanaka, and A. P. Mills, Jr., Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.95.195006 95, 195006 (2005).
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(2005)
Phys. Rev. Lett.
, vol.95
, pp. 195006
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Cassidy, D.B.1
Deng, S.H.M.2
Greaves, R.G.3
Maruo, T.4
Nishiyama, N.5
Snyder, J.B.6
Tanaka, H.K.M.7
Mills Jr., A.P.8
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29
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4243651056
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PRLTAO 0031-9007 10.1103/PhysRevLett.54.1702
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K. G. Lynn, A. P. Mills, R. N. West, S. Berko, K. F. Canter, and L. O. Roellig, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.54.1702 54, 1702 (1985).
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(1985)
Phys. Rev. Lett.
, vol.54
, pp. 1702
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Lynn, K.G.1
Mills, A.P.2
West, R.N.3
Berko, S.4
Canter, K.F.5
Roellig, L.O.6
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30
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4243315081
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PRLTAO 0031-9007 10.1103/PhysRevLett.44.1330
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K. G. Lynn, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.44.1330 44, 1330 (1980).
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(1980)
Phys. Rev. Lett.
, vol.44
, pp. 1330
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Lynn, K.G.1
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31
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0000702734
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PRBMDO 0163-1829 10.1103/PhysRevB.44.5791
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A. P. Mills, Jr., E. D. Shaw, M. Leventhal, R. J. Chichester, and D. M. Zuckerman, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.44.5791 44, 5791 (1991).
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(1991)
Phys. Rev. B
, vol.44
, pp. 5791
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Mills Jr., A.P.1
Shaw, E.D.2
Leventhal, M.3
Chichester, R.J.4
Zuckerman, D.M.5
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33
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0001146406
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PLRAAN 1050-2947 10.1103/PhysRevA.26.490
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A. P. Mills, Jr. and R. J. Wilson, Phys. Rev. A PLRAAN 1050-2947 10.1103/PhysRevA.26.490 26, 490 (1982).
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(1982)
Phys. Rev. A
, vol.26
, pp. 490
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Mills Jr., A.P.1
Wilson, R.J.2
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34
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0003998388
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The total energy deposited by a fully compressed positron pulse is U=1.5× 107 ×1500 eV×1.6× 10-19 J eV=3.6× 10-9 J. The total volume into which this energy is deposited is V=π× (0.02)2 ×2.5× 10-6 cm=3× 10-9 cm3. The heat capacity of Al at 300 K is Cp =5.82 cal K mole=24.4 J K 27 g=2.44 J K-1 cm-3. The temperature rise neglecting heat conduction is then given by ΔT=U V Cp =3.6× 10-9 J (2.44 J K-1 ×3× 10-9 cm3) =0.5 K. This is the maximum temperature variation. In reality the heat will diffuse during the 1 ns implantation time and the actual surface temperature would be much less than this. The Al heat capacity was taken from the CSC Press, Boca Raton, edited by R. C. Weast (66th ed.
-
The total energy deposited by a fully compressed positron pulse is U=1.5× 107 ×1500 eV×1.6× 10-19 J eV=3.6× 10-9 J. The total volume into which this energy is deposited is V=π× (0.02)2 ×2.5× 10-6 cm=3× 10-9 cm3. The heat capacity of Al at 300 K is Cp =5.82 cal K mole=24.4 J K 27 g=2.44 J K-1 cm-3. The temperature rise neglecting heat conduction is then given by ΔT=U V Cp =3.6× 10-9 J (2.44 J K-1 ×3× 10-9 cm3) =0.5 K. This is the maximum temperature variation. In reality the heat will diffuse during the 1 ns implantation time and the actual surface temperature would be much less than this. The Al heat capacity was taken from the Handbook of Chemistry and Physics, 66th ed., edited by, R. C. Weast, (CSC Press, Boca Raton, 1985).
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(1985)
Handbook of Chemistry and Physics
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35
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4244092620
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The maximum slope of a fd vs T curve is 0.03 200 °C=1.5× 10-4 [10.1103/PhysRevLett.41.1828 0031-9007 PRLTAO
-
The maximum slope of a fd vs T curve is 0.03 200 °C=1.5× 10-4 [A. P. Mills, Jr., Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.41.1828 41, 1828 (1978)] which gives a Ps delayed fraction thermally induced by beam impact of ∼7.5× 10-5 which is an upper limit and is more than 10 times smaller than the effect we observe.
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(1978)
Phys. Rev. Lett.
, vol.41
, pp. 1828
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Mills Jr., A.P.1
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36
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4243989530
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Large shifts in the work function have been observed on Cu surfaces due to a partial coverage of Cs. [PRLTAO 0031-9007 10.1103/PhysRevLett.68.2378
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Large shifts in the work function have been observed on Cu surfaces due to a partial coverage of Cs. [C. A. R. Koymen, K. H. Lee, D. Mehl, A. Weiss, and K. O. Jensen, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.68.2378 68, 2378 (1992).] The shifts do not simply imply a change in the surface dipole potential, but must involve changes in the width and/or depth of the potential well seen by the surface positrons.
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(1992)
Phys. Rev. Lett.
, vol.68
, pp. 2378
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Koymen, C.A.R.1
Lee, K.H.2
Mehl, D.3
Weiss, A.4
Jensen, K.O.5
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37
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27744520126
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See, for example, edited by J. T. Devreese and F. P. Peters (Plenum, New York
-
See, for example, P. M. Platzman, in The Physics of the Two-Dimensional Electron Gas, edited by, J. T. Devreese, and, F. P. Peters, (Plenum, New York, 1986), pp. 97-130.
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(1986)
The Physics of the Two-Dimensional Electron Gas
, pp. 97-130
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Platzman, P.M.1
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39
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0000703506
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APHYCC 0340-3793 10.1007/BF00899716
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A. P. Mills, Jr., Appl. Phys. APHYCC 0340-3793 10.1007/BF00899716 23, 189 (1980).
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(1980)
Appl. Phys.
, vol.23
, pp. 189
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Mills Jr., A.P.1
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40
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0005428866
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PRBMDO 0163-1829 10.1103/PhysRevB.34.442
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P. J. Schultz, E. M. Gullikson, and A. P. Mills, Jr., Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.34.442 34, 442 (1986).
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(1986)
Phys. Rev. B
, vol.34
, pp. 442
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Schultz, P.J.1
Gullikson, E.M.2
Mills Jr., A.P.3
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41
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0001271286
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Careful measurements via low energy electron diffraction (LEED) might reveal variations in the surface structure, but would not be directly sensitive to hydrogen contamination. On the other hand, positron diffraction might reveal hydrogen on an Al surface: PRBMDO 0163-1829 10.1103/PhysRevB.48.2400
-
Careful measurements via low energy electron diffraction (LEED) might reveal variations in the surface structure, but would not be directly sensitive to hydrogen contamination. On the other hand, positron diffraction might reveal hydrogen on an Al surface: X. M. Chen, K. F. Canter, C. B. Duke, A. Paton, D. L. Lessor, and W. K. Ford, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.48.2400 48, 2400 (1993).
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(1993)
Phys. Rev. B
, vol.48
, pp. 2400
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Chen, X.M.1
Canter, K.F.2
Duke, C.B.3
Paton, A.4
Lessor, D.L.5
Ford, W.K.6
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42
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0000696952
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PRLTAO 0031-9007 10.1103/PhysRevLett.80.1876
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K. Varga, J. Usukura, and Y. Suzuki, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.80.1876 80, 1876 (1998).
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(1998)
Phys. Rev. Lett.
, vol.80
, pp. 1876
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Varga, K.1
Usukura, J.2
Suzuki, Y.3
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