1989
DOI: 10.1007/978-1-4613-0541-5_4
|View full text |Cite
|
Sign up to set email alerts
|

Rapid Thermal Annealing - Theory and Practice

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
21
0

Year Published

1993
1993
2023
2023

Publication Types

Select...
5
3

Relationship

0
8

Authors

Journals

citations
Cited by 37 publications
(22 citation statements)
references
References 5 publications
0
21
0
Order By: Relevance
“…Any process that involves fast heating and cooling rates could be placed in this category. Review papers [14][15][16] described the advantages of isothermal heating (lamp, resistance, and e-beam heating, 1-100 s processing time) over thermal flux (scanned continuous wave (cw) laser, e-beam, 0.1-10 ms processing time) and adiabatic heating (pulsed beam or laser, 1-1000 ns processing time) to semiconductor manufacturing [17,18]. However, the demands of RTP systems for material modification are quite different from those used in microelectronics applications.…”
Section: The Rtp Techniquementioning
confidence: 99%
“…Any process that involves fast heating and cooling rates could be placed in this category. Review papers [14][15][16] described the advantages of isothermal heating (lamp, resistance, and e-beam heating, 1-100 s processing time) over thermal flux (scanned continuous wave (cw) laser, e-beam, 0.1-10 ms processing time) and adiabatic heating (pulsed beam or laser, 1-1000 ns processing time) to semiconductor manufacturing [17,18]. However, the demands of RTP systems for material modification are quite different from those used in microelectronics applications.…”
Section: The Rtp Techniquementioning
confidence: 99%
“…Because is weakly dependent on temperature, instantaneous spatial temperature variations across wafers at given times are expected to be small enough ( 200 K) so that spatial variations in thermal conductivity may be ignored [4]. Thus, (1) may be reduced to (3) The initial and boundary conditions for the system described above are at (4) at (5) at (6) at (7) at (8) where is the wafer surface absorptivity, is the wafer surface emissivity, is the emissivity for the radiant heat losses at the wafer edges, and W cm K is the Stefan-Boltzmann constant. Note that absorptivity and emissivity may depend on wafer temperature, position, and radiant spectral wavelength [16], [17].…”
Section: Thermal Modelmentioning
confidence: 99%
“…It is known that incident-heat-flux profiles (energy distributions) in RTP systems must be nonuniform across wafers to ensure temperature uniformity at all times because of heat losses at wafer edges. Hill and Jones [3] investigated the temperature uniformity of a 150-mm (6-in) wafer in which the intensity was linearly enhanced to a maximum of 8% over the last 15 mm of the wafer. Kakoschke et al [4] presented a wafer-heating theory for estimating the edge-heating compensation required vertically and laterally to ensure temperature Publisher Item Identifier S 0894-6507(01)03520-5.…”
Section: Introductionmentioning
confidence: 99%
“…2), spatial temperature variations across wafers at a certain time are expected to be small enough ( 200 K) so that spatial variations in thermal conductivity may be ignored [5]. Equation (1) is thus reduced to (3) The initial and boundary conditions for the system mentioned above are at (4) at (5) at (6) where is the emissivity for radiant heat loss emitted from the wafer edge. We may assume without loss of generality that the incident heat flux on both sides during processing is equal, i.e.,…”
Section: Thermal Modelmentioning
confidence: 99%
“…Hill and Jones [4] investigated thermal uniformity with a uniform intensity field and one in which the intensity was linearly enhanced to a maximum of 8% vertically over the last 15 mm of a 6-in wafer. Kakoschke et al [5] evaluated enhanced illumination intensities at wafer peripheries vertically and laterally for a compensation of edge heat losses during processing.…”
Section: Introductionmentioning
confidence: 99%