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1
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85038334729
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edited by D. L. Beke, Landolt-Börnstein, New Series, III/33A (Springer, Berlin, 1998)
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Diffusion in Semiconductors, edited by D. L. Beke, Landolt-Börnstein, New Series, Vol. III/33A (Springer, Berlin, 1998).
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2
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0000514669
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W. Schröter, VCH, Weinheim, and, in, edited by, p
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U. Gösele and T Y. Tan, in Electronic Structure and Properties of Semiconductors, edited by W. Schröter (VCH, Weinheim, 1991), p. 97.
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(1991)
Electronic Structure and Properties of Semiconductors
, pp. 97
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Gösele, U.1
Tan, T.Y.2
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4
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0001527312
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M. Jacob, P. Pichler, H. Ryssel, and R. Falster, J. Appl. Phys.82, 182 (1997).
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(1997)
J. Appl. Phys.
, vol.82
, pp. 182
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Jacob, M.1
Pichler, P.2
Ryssel, H.3
Falster, R.4
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7
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0032096170
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D. Wörle, H. Grünleitner, V. Demuth, C. Kumpf, H P. Strunk, E. Burkel, and M. Schulz, Appl. Phys. A: Mater. Sci. Process.A66, 629 (1998).
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(1998)
Appl. Phys. A: Mater. Sci. Process.
, vol.A66
, pp. 629
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Wörle, D.1
Grünleitner, H.2
Demuth, V.3
Kumpf, C.4
Strunk, H.P.5
Burkel, E.6
Schulz, M.7
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8
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85038302293
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This layer has been taken into account in the diffusion depth coordinate
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This layer has been taken into account in the diffusion depth coordinate.
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9
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85038316672
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Our simulations show that diffusion, the wafer cannot account for the large amount of backside Ir
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Our simulations show that diffusion through the wafer cannot account for the large amount of backside Ir.
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10
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84934155988
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W. Jüngling, P. Pilcher, S. Selbstherr, E. Guerrero, and H W. Plötzel, IEEE Trans. Electron DevicesED-32, 156 (1985).
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(1985)
IEEE Trans. Electron Devices
, vol.ED-32
, pp. 156
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Jüngling, W.1
Pilcher, P.2
Selbstherr, S.3
Guerrero, E.4
Plötzel, H.W.5
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12
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0033908116
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A. Giese, H. Bracht, N A. Stolwijk, and D. Baither, Mater. Sci. Eng., B71, 160 (2000).
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(2000)
Mater. Sci. Eng., B
, vol.71
, pp. 160
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Giese, A.1
Bracht, H.2
Stolwijk, N.A.3
Baither, D.4
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13
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85038338082
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For fixed (formula presented) (formula presented) settles according to (formula presented) based on mass action law and (formula presented). Conversely, fitting of (formula presented) also determines (formula presented)
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For fixed (formula presented) (formula presented) settles according to (formula presented) based on mass action law and (formula presented). Conversely, fitting of (formula presented) also determines (formula presented).
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14
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85038337440
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We checked that the alternative modeling condition (formula presented) with (formula presented) as adjustable flux limitation parameter for (formula presented) leads to essentially the same quantitative results. In this approach (formula presented) increases monotonically with diffusion time, and so does (formula presented)
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We checked that the alternative modeling condition (formula presented) with (formula presented) as adjustable flux limitation parameter for (formula presented) leads to essentially the same quantitative results. In this approach (formula presented) increases monotonically with diffusion time, and so does (formula presented).
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15
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85038297847
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(formula presented) has been omitted in Table I since it does not represent a basic physical property
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(formula presented) has been omitted in Table I since it does not represent a basic physical property.
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18
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0016975751
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Fiz. Tekh. Poluprovodn., 1418 (1976)
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S A. Azimov, B V. Umarov, and M S. Yunusov, Fiz. Tekh. Poluprovodn. 10, 1418 (1976) [Sov. Phys. Semicond.10, 842 (1976)].
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(1976)
Sov. Phys. Semicond.
, vol.10
, pp. 842
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Azimov, S.A.1
Umarov, B.V.2
Yunusov, M.S.3
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19
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0029376294
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W. Lerch, N A. Stolwijk, H. Mehrer, and Ch. Poisson, Semicond. Sci. Technol.10, 1257 (1995).
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(1995)
Semicond. Sci. Technol.
, vol.10
, pp. 1257
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Lerch, W.1
Stolwijk, N.A.2
Mehrer, H.3
Poisson, C.4
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20
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85038311403
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In fact, for (formula presented) the effective diffusivity for both (formula presented) and (formula presented) is given by (formula presented)
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In fact, for (formula presented) the effective diffusivity for both (formula presented) and (formula presented) is given by (formula presented).
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21
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85038314722
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The, -controlled diffusivity prevails for (formula presented) and reads (formula presented) producing convex profiles when plotted as (formula presented) vs
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The I-controlled diffusivity prevails for (formula presented) and reads (formula presented) producing convex profiles when plotted as (formula presented) vs x.
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