Apparatus and method for online and real-time detection of temperature of epitaxial wafer
10908024 ยท 2021-02-02
Assignee
Inventors
- Dong YAN (Beijing, CN)
- Chengmin Li (Beijing, CN)
- Linzi Wang (Beijing, CN)
- Jianpeng Liu (Beijing, CN)
- Longmao Ye (Beijing, CN)
Cpc classification
G01J5/0007
PHYSICS
International classification
Abstract
An apparatus and a method for online and real-time detection of a temperature of an epitaxial wafer (4) belong to the technical field of semiconductor detection. The apparatus comprises a MOCVD reaction chamber (1), a light source (6), a beam splitter (7), a reference light detector (8), a reflected light detector (9) and a data acquisition unit (10). The method, on the basis of the apparatus, can obtain a thermal radiation attenuation factor caused by a coating of a reactor chamber window and a reflectance attenuation factor caused by the coating of the reactor chamber window for the epitaxial wafer (4). The apparatus and method can eliminate influence of the coating of the reactor chamber window on an online and real-time temperature detection value, thereby improving the accuracy of the online and real-time temperature detection value.
Claims
1. An apparatus for online and real-time detection of a temperature of an epitaxial wafer, comprising a MOCVD reaction chamber, a light source, a beam splitter, a reference light detector, a reflected light detector and a data acquisition unit, wherein, the MOCVD reaction chamber is provided with a graphite susceptor therein, the graphite susceptor being able to rotate and used to bear the epitaxial wafer, and a top of the MOCVD reaction chamber is provided with a reaction chamber window for enabling light to pass therethrough; the light source is configured to generate a light beam; the beam splitter is configured to split the light beam received from the light source into two beams, and wherein one of the two beams after entering the reference light detector, forms a first path of electrical signal, and the other of the two beams passes through the reaction chamber window and then strikes on the epitaxial wafer and forms a reflected light beam after being reflected by the epitaxial wafer, the reflected light beam forming a second path of electrical signal after passing through the reflected light detector; and the data acquisition unit is configured to acquire the first path of electrical signal and the second path of electrical signal.
2. The apparatus of claim 1, further comprising a light source switch control circuit and/or a data processing unit, the light source switch control circuit being used to control on and off of the light source, the data processing unit being configured to process signals acquired by the data acquisition unit.
3. The apparatus of claim 1, further comprising a CPU, the CPU is configured to control the switch control circuit so as to control the on and off of the light source, and further to process signals acquired by the data acquisition unit.
4. The apparatus of claim 1, wherein when the light source is turned on, the second path of electrical signal is a sum of a reflected light intensity of the epitaxial wafer and a thermal radiation intensity of the epitaxial wafer; and when the light source is turned off, the second path of electrical signal is a thermal radiation intensity of the epitaxial wafer.
5. A method for online and real-time detection of a temperature of an epitaxial wafer based on the apparatus of claim 1, comprising: Step 1: obtaining a reflected light intensity of the epitaxial wafer and a thermal radiation intensity of the epitaxial wafer respectively based on a second path of electrical signal detected by a reflected light detector when a light source is turned on and a second path of electrical signal detected by the reflected light detector when the light source is turned off,
Irefl=IonIoff
L(,T)=Ioff where, Ion is the second path of electrical signal detected by the reflected light detector when the light source is turned on, Ioff is the second path of electrical signal detected by the reflected light detector when the light source is turned off, Irefl is the reflected light intensity of the epitaxial wafer, L (, T) is the thermal radiation intensity of the epitaxial wafer; Step 2: obtaining a reflectance of the epitaxial wafer based on the reflected light intensity of the epitaxial wafer and a reference light intensity,
T.sub.T={square root over (T.sub.R)}(3) where, TT is the thermal radiation attenuation factor caused by the coating of the reaction chamber window, TR is the reflectance attenuation factor caused by the coating of the reaction chamber window; Step 5: calculating a black-body thermal radiation value Pb (, T) of the epitaxial wafer based on the thermal radiation intensity L (, T) of the epitaxial wafer, the reflectance R of the epitaxial wafer, the thermal radiation attenuation factor TT caused by the coating of the reaction chamber window, and the reflectance attenuation factor TR caused by the coating of the reaction chamber window,
6. The method of claim 5, further comprising a step of selecting to obtain the thermal emissivity (R/T.sub.R) of the epitaxial wafer, wherein when the coating of the reaction chamber window is formed as an ideal opaque, smooth and flat surface,
(R/T.sub.R)=1R/T.sub.R where, R is the reflectance of the epitaxial wafer, TR is the reflectance attenuation factor caused by the coating of the reaction chamber window, (R/T.sub.R) is the thermal emissivity of the epitaxial wafer.
7. The method of claim 5, further comprising a step of selecting to obtain the thermal emissivity (R/T.sub.R) of the epitaxial wafer, wherein when the reaction chamber window is coated, and the substrate is transparent and single-side polished,
(R/T.sub.R)=.sub.carr(1R/T.sub.R)(1R.sub.diff){1+R/T.sub.R*R.sub.diff+(1.sub.carr)[(R.sub.diff+R/T.sub.R(1R.sub.diff).sup.2)]} where, (R/T.sub.R) is the thermal emissivity of the epitaxial wafer, R is the reflectance of the epitaxial wafer, R.sub.diff is a scattering rate of a non-smooth substrate, .sub.carr is the thermal emissivity of the graphite susceptor, and TR is the reflectance attenuation factor caused by the coating of the reaction chamber window.
8. The method of claim 5, further comprising a step of obtaining the ratio of light intensity m of the reference light to the incident light, the ratio of light intensity m is obtained by a formula:
9. The apparatus of claim 2, wherein when the light source is turned on, the second path of electrical signal is a sum of a reflected light intensity of the epitaxial wafer and a thermal radiation intensity of the epitaxial wafer; and when the light source is turned off, the second path of electrical signal is a thermal radiation intensity of the epitaxial wafer.
10. The apparatus of claim 3, wherein when the light source is turned on, the second path of electrical signal is a sum of a reflected light intensity of the epitaxial wafer and a thermal radiation intensity of the epitaxial wafer; and when the light source is turned off, the second path of electrical signal is a thermal radiation intensity of the epitaxial wafer.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1)
(2)
(3)
(4)
(5)
(6)
(7)
(8)
DETAILED DESCRIPTION OF THE INVENTION
(9) The present invention will be described in detail below in conjunction with the drawings and specific embodiments in order to understand the invention thoroughly.
(10) Referring to
(11) Referring to
(12) The light source 6 is used for generating a light beam.
(13) The beam splitter 7 may split the light beam received from the light source 6 into two beams, one of which after entering the reference light detector 8, forms a first path of electrical signal representing a reference light intensity, and the other of which passes through the reaction chamber window 5 and then strikes on the epitaxial wafer 4, and is reflected by the epitaxial wafer 4 to form a reflected light beam. The reflected light beam forms a second path of electrical signal after passing through the reflected light detector 9.
(14) The data acquisition unit 10 is configured to acquire an identity information of the epitaxial wafer 4, the first path of electrical signal, and the second path of electrical signal.
(15) Referring to
(16) Referring to
(17) When the light source 6 is turned on, the second path of electrical signal is a sum of a reflected light intensity of the epitaxial wafer 4 and a thermal radiation intensity of the epitaxial wafer 4. When the light source 6 is turned off, the second path of electrical signal is a thermal radiation intensity of the epitaxial wafer 4.
(18) Referring to
(19) Step 1: obtaining a reflected light intensity of the epitaxial wafer 4 and a thermal radiation intensity of the epitaxial wafer 4 based on a second path of electrical signal detected by a reflected light detector 9 when a light source 6 is turned on and a second path of electrical signal detected by the reflected light detector 9 when the light source 6 is turned off, respectively,
I.sub.refl=I.sub.onI.sub.off
L(,T)=I.sub.off
(20) where,
(21) I.sub.on is a second path of electrical signal detected by the reflected light detector 9 when the light source 6 is turned on,
(22) I.sub.off is a second path of electrical signal detected by the reflected light detector 9 when the light source 6 is turned off,
(23) I.sub.refl is a reflected light intensity of the epitaxial wafer 4,
(24) L(, T) is a thermal radiation intensity of the epitaxial wafer 4;
(25) Step 2: obtaining a reflectance of the epitaxial wafer 4 based on the reflected light intensity of the epitaxial wafer 4 and a reference light intensity,
(26)
(27) where
(28) R is a reflectance of the epitaxial wafer,
(29) m is a ratio of light intensity of a reference light to an incident light,
(30) I.sub.refl is a reflected light intensity of the epitaxial wafer,
(31) I.sub.refe is a reference light intensity;
(32) Step 3: obtaining a reflectance attenuation factor caused by a coating of a reaction chamber window 5 based on a reflectance of the epitaxial wafer 4 and an ideal reflectance of the epitaxial wafer 4,
(33)
(34) where,
(35) T.sub.R is a reflectance attenuation factor caused by the coating of the reaction chamber window 5,
(36) R is a reflectance of the epitaxial wafer 4,
(37) R.sub.0 is an ideal reflectance of the epitaxial wafer 4;
(38) Step 4: obtaining a thermal radiation attenuation factor caused by the coating of the reaction chamber window 5 based on the reflectance attenuation factor caused by the coating of the reaction chamber window 5,
T.sub.T={square root over (T.sub.R)}(3)
(39) where,
(40) T.sub.T is a thermal radiation attenuation factor caused by the coating of the reaction chamber window 5,
(41) T.sub.R is a reflectance attenuation factor caused by the coating of the reaction chamber window 5;
(42) Step 5: calculating a black-body thermal radiation value P.sub.b(, T) of the epitaxial wafer 4 based on the thermal radiation intensity L(, T) of the epitaxial wafer 4, the reflectance R of the epitaxial wafer 4, the thermal radiation attenuation factor T.sub.T caused by the coating of the reaction chamber window 5, and the reflectance attenuation factor T.sub.R caused by the coating of the reaction chamber window 5,
(43)
(44) where,
(45) P.sub.b(, T) is a black-body thermal radiation value,
(46) L(, T) is a thermal radiation intensity of the epitaxial wafer 4,
(47) R is a reflectance of the epitaxial wafer 4,
(48) T.sub.T is a thermal radiation attenuation factor caused by the coating of the reaction chamber window 5,
(49) T.sub.R is a reflectance attenuation factor caused by the coating of the reaction chamber window 5,
(50) (R/T.sub.R) is a thermal emissivity of the epitaxial wafer 4;
(51) Step 6: obtaining a temperature T of the epitaxial wafer 4 based on a correspondence relationship between the black-body thermal radiation value P.sub.b(, T) and the temperature T of the epitaxial wafer 4,
(52)
(53) where,
(54) P.sub.b(, T) is an ideal black-body thermal radiation value,
(55) h is Planck constant,
(56) k is Boltzmann constant,
(57) c is light speed,
(58) is wavelength,
(59) T is temperature.
(60) In some embodiments, as a specific step of obtaining the thermal emissivity (R/T.sub.R) of the epitaxial wafer 4, the method for online and real-time detection of a temperature of an epitaxial wafer according to an embodiment of the present invention may further comprise a step of selecting to obtain the thermal emissivity (R/T.sub.R) of the epitaxial wafer 4.
(61) In some embodiments, when the coating of the reaction chamber window 5 is formed as an ideal opaque, smooth and flat surface,
(R/T.sub.R)=1R/T.sub.R
(62) where,
(63) R is a reflectance of the epitaxial wafer,
(64) T.sub.R is a reflectance attenuation factor caused by the coating of the reaction chamber window,
(65) (R/T.sub.R) is a thermal emissivity of the epitaxial wafer.
(66) In some embodiments, when the reaction chamber window is coated, and the substrate is transparent and single-side polished,
(R/T.sub.R)=.sub.carr(1R/T.sub.R)(1R.sub.diff){1+R/T.sub.R*R.sub.diff+(1.sub.carr)[(R.sub.diff+R/T.sub.R(1R.sub.diff).sup.2)]}
(67) where,
(68) (R/T.sub.R) is a thermal emissivity of the epitaxial wafer 4,
(69) R is a reflectance of the epitaxial wafer 4,
(70) R.sub.diff is a scattering rate of a non-smooth substrate,
(71) .sub.carr is a thermal emissivity of a graphite susceptor,
(72) T.sub.R is a reflectance attenuation factor caused by the coating of the reaction chamber window 5.
(73) In an embodiment, as a specific step of obtaining the ratio of light intensity m of a reference light to an incident light, the method for online and real-time detection of a temperature of an epitaxial wafer according to the present invention may further comprise a step of obtaining a ratio of light intensity m of the reference light to the incident light, and the ratio of light intensity m is obtained by the following formula:
(74)
(75) where,
(76) R.sub.standard is a reflectance of an epitaxial wafer having a standard reflectance,
(77) m is a ratio of the light intensity of the reference light to the incident light,
(78) I.sub.refl is a reflected light intensity of the epitaxial wafer 4,
(79) I.sub.refe is a reference light intensity.
(80) The apparatus and the method for online and real-time detection of a temperature of an epitaxial wafer according to the present disclosure can obtain the thermal radiation attenuation factor T.sub.T caused by the coating of the reaction chamber window 5 and the reflectance attenuation factor T.sub.R caused by the coating of the reaction chamber window 5 for the epitaxial wafer 4, apply the two attenuation factors T.sub.T and T.sub.R to a calculation process of the black-body thermal radiation value of the epitaxial wafer 4, and take advantage of the relationship between the black-body thermal radiation value of the epitaxial wafer 4 obtained by calculation and the temperature of the epitaxial wafer 4, thereby eliminating the effect of the coating of the reaction chamber window 5 on the online and real-time temperature detection value and improving the accuracy of the online and real-time temperature detection value.
(81) The above embodiments have described the objects, the technical solutions and the advantageous effects of the invention in detail. It should be appreciated that the above embodiments are only specific embodiments of the invention and are not intended to limit the invention. Any modifications, equivalent substitutions, improvements, etc., made within the spirit and principle of the invention, are intended to be included within the scope of the invention.