-
5
-
-
0020495861
-
-
S. Duncan, R. Smith, D. E. Sykes, and J. M. Walls, Vacuum 34, 145 (1984).
-
(1984)
Vacuum
, vol.34
, pp. 145
-
-
Duncan, S.1
Smith, R.2
Sykes, D.E.3
Walls, J.M.4
-
6
-
-
84953679766
-
-
F. A. Stevie, P. M. Kahora. D. S. Simons, and P. Chi, J. Vac. Sci. Technol. A 6, 76 (1988).
-
(1988)
J. Vac. Sci. Technol. A
, vol.6
, pp. 76
-
-
Stevie, F.A.1
Kahora, P.M.2
Simons, D.S.3
Chi, P.4
-
8
-
-
0000402110
-
-
K. Elst, W. Vandervorst, J. Alay, J. Snauwaert, and L. Hellemans, J. Vac. Sci. Technol. B 11, 1968 (1993). The ion energy quoted in this article relates to the beam propagating along the gun column, i.e., before retardation due to the target bias of 4.5 kV.
-
(1993)
J. Vac. Sci. Technol. B
, vol.11
, pp. 1968
-
-
Elst, K.1
Vandervorst, W.2
Alay, J.3
Snauwaert, J.4
Hellemans, L.5
-
11
-
-
0001590230
-
-
K. Elst and W. Vandervorst, J. Vac. Sci. Technol. A 12, 3205 (1994). The quoted angles do not take into account the deflection prior to retardation, see Ref. 12. The energy for the uncorrected angle θ' = 36° was not specified in the text, but may be calculated from θ' as 12 keV.
-
(1994)
J. Vac. Sci. Technol. A
, vol.12
, pp. 3205
-
-
Elst, K.1
Vandervorst, W.2
-
12
-
-
0024764767
-
-
M. Meuris, P. De Bisschop, J. F. Leclair, and W. Vandervorst, Surf. Interface Anal. 14, 739 (1989).
-
(1989)
Surf. Interface Anal.
, vol.14
, pp. 739
-
-
Meuris, M.1
De Bisschop, P.2
Leclair, J.F.3
Vandervorst, W.4
-
13
-
-
11744323004
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+ signal increases by a few percent at a depth of about 1.5 μm. This implies that ripple formation is not really disappearing at very high pressures but difficult to identify, probably because of a reduced growth rate
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+ signal increases by a few percent at a depth of about 1.5 μm. This implies that ripple formation is not really disappearing at very high pressures but difficult to identify, probably because of a reduced growth rate.
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-
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14
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11744299949
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M. G. Dowsett, N. S. Smith, R. Brigdeland, D. Richards, A. C. Lovejoy, and P. Pedrick, in Ref. 4, p. 367
-
M. G. Dowsett, N. S. Smith, R. Brigdeland, D. Richards, A. C. Lovejoy, and P. Pedrick, in Ref. 4, p. 367.
-
-
-
-
15
-
-
11744272784
-
-
Research Triangle Park, NC. Book of Extended Abstracts, edited by M. Current et al., Paper No. 15
-
M. G. Dowsett and D. P. Chu, Fourth International Worshop on Measurement, Characterization and Modeling of Ultra-Shallow Doping Profiles in Semiconductors, Research Triangle Park, NC. 1997. Book of Extended Abstracts, edited by M. Current et al., Paper No. 15.
-
(1997)
Fourth International Worshop on Measurement, Characterization and Modeling of Ultra-Shallow Doping Profiles in Semiconductors
-
-
Dowsett, M.G.1
Chu, D.P.2
-
19
-
-
84912907721
-
-
M. Meuris, W. Vandervorst, and J. Jackman, J, Vac. Sci. Technol. A 9, 1482 (1991).
-
(1991)
J, Vac. Sci. Technol. A
, vol.9
, pp. 1482
-
-
Meuris, M.1
Vandervorst, W.2
Jackman, J.3
-
20
-
-
84957231263
-
-
W. Vandervorst, F. R. Shepherd, J. Newman, B. F. Phillips, and J. Remmerie, J. Vac. Sci. Technol. A 3, 1359 (1985).
-
(1985)
J. Vac. Sci. Technol. A
, vol.3
, pp. 1359
-
-
Vandervorst, W.1
Shepherd, F.R.2
Newman, J.3
Phillips, B.F.4
Remmerie, J.5
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25
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11744283802
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note
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One of the referees pointed out that, on PHI quadrupole based SIMS systems, the uncertainty in impact angle is closer to ±5°.
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26
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11744295678
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Ph.D. thesis, Universiteit Antwerpen, Belgium
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r=41°±3° for both faces, it is impossible that the root-mean-square amplitude and the wave length of the ripples were almost the same, as implied by Figs. 6.4.b and 1(a) for depths between 5 and 12 μm. Inspection of the quantified 3D AFM images in this thesis shows that the ratio of the mean ripple height h to the ripple spacing s amounted to 0.4±0.05, in accordance with Eq. (1).
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(1993)
-
-
Elst, K.1
-
27
-
-
0003412161
-
-
Pergamon, New York
-
J. F. Ziegler, J. P. Biersack, and U. Littmark, The Stopping and Range of Ions in Solids, Vol. 1 (Pergamon, New York, 1985).
-
(1985)
The Stopping and Range of Ions in Solids
, vol.1
-
-
Ziegler, J.F.1
Biersack, J.P.2
Littmark, U.3
-
28
-
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0346239376
-
-
R. D. Barlow, M. G. Dowsett, H. S. Fox, R. A. A. Kubiak, and S. M. Newstead, Nucl. Instrum. Methods Phys. Res. B 72, 442 (1992).
-
(1992)
Nucl. Instrum. Methods Phys. Res. B
, vol.72
, pp. 442
-
-
Barlow, R.D.1
Dowsett, M.G.2
Fox, H.S.3
Kubiak, R.A.A.4
Newstead, S.M.5
-
29
-
-
84953677167
-
-
E.-H. Cirlin, J. J. Vajo, T. C. Hasenberg, and R. J. Hauenstein, J. Vac. Sci. Technol. A 8, 4101 (1990).
-
(1990)
J. Vac. Sci. Technol. A
, vol.8
, pp. 4101
-
-
Cirlin, E.-H.1
Vajo, J.J.2
Hasenberg, T.C.3
Hauenstein, R.J.4
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