Method for fabrication a multi-well amorphous selenium detector
10868202 ยท 2020-12-15
Assignee
Inventors
Cpc classification
H01L31/02161
ELECTRICITY
H01L31/022408
ELECTRICITY
H01L27/14692
ELECTRICITY
H01L31/107
ELECTRICITY
H01L27/14696
ELECTRICITY
International classification
H01L21/06
ELECTRICITY
H01L31/107
ELECTRICITY
Abstract
Provided is a field shaping multi-well detector and method of fabrication thereof. The detector is configured by depositing a pixel electrode on a substrate, depositing a first dielectric layer, depositing a first conductive grid electrode layer on the first dielectric layer, depositing a second dielectric layer on the first conductive grid electrode layer, depositing a second conductive grid electrode layer on the second dielectric layer, depositing a third dielectric layer on the second conductive grid electrode layer, depositing an etch mask on the third dielectric layer. Two pillars are formed by etching the third dielectric layer, the second conductive grid electrode layer, the second dielectric layer, the first conductive grid electrode layer, and the first dielectric layer. A well between the two pillars is formed by etching to the pixel electrode, without etching the pixel electrode, and the well is filled with a-Se.
Claims
1. A method of fabricating a multi-well amorphous selenium (a-Se) detector, comprising: depositing a pixel electrode adjacent to a substrate; depositing a first dielectric layer; depositing a first conductive grid electrode layer on the first dielectric layer; depositing a second dielectric layer on the first conductive grid electrode layer; depositing a second conductive grid electrode layer on the second dielectric layer; depositing a third dielectric layer on the second conductive grid electrode layer; depositing an etch mask on the third dielectric layer; performing a first etching to form at least two pillars with at least one well therebetween; depositing an oxide dielectric layer on the at least two pillars and on a bottom of the at least one well; and performing a second etching to remove the oxide dielectric layer from the bottom of the at least one well.
2. The method of claim 1, wherein the first etching is performed from the third dielectric layer, to the second conductive grid electrode layer, to the second dielectric layer, to the first conductive grid electrode layer, to the first dielectric layer, and to the pixel electrode.
3. The method of claim 1, wherein the first etching is anisotropic.
4. The method of claim 1, wherein the first etching does not etch the pixel electrode.
5. The method of claim 1, wherein the second etching does not remove the oxide dielectric layer from sides of the at least two pillars with the at least one well.
6. The method of claim 1, wherein the second etching does not etch the pixel electrode.
7. The method of claim 1, wherein each of the at least two pillars includes the first conductive grid electrode layer and the second conductive grid electrode layer, forming on opposite sides of the at least one well a pair of first conductive grid electrode layers and a pair of second conductive grid electrode layers.
8. The method of claim 7, wherein the pair of first conductive grid electrode layers are spaced apart from the pixel electrode by a first distance.
9. The method of claim 8, wherein the pair of second conductive grid electrode layers are spaced apart from the pixel electrode by a second distance.
10. The method of claim 9, wherein the first distance is different from the second distance.
11. The method of claim 7, wherein the oxide dielectric layer fully encapsulates each of the pair of first conductive grid electrode layers.
12. The method of claim 7, wherein the oxide dielectric layer fully encapsulates each of the pair of second conductive grid electrode layers.
13. The method of claim 7, wherein the pair of first conductive grid electrode layers align with the pair of second conductive grid electrode layers, without aligning the first conductive grid electrode layer and the second conductive grid electrode layer before performing the first etching.
14. The method of claim 1, wherein the first conductive grid electrode layer and the second conductive grid electrode layer are not patterned before stacking on the first dielectric layer or on the second dielectric layer, respectively.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1) The above and other aspects, features and advantages of certain embodiments of the present invention will be more apparent from the following detailed description taken in conjunction with the accompanying drawings, in which:
(2)
(3)
(4)
(5)
(6)
(7)
(8)
(9)
(10)
DETAILED DESCRIPTION OF EMBODIMENTS OF THE INVENTION
(11) The following detailed description of certain embodiments of the present invention will be made with reference to the accompanying drawings. In describing the invention, explanation about related functions or constructions known in the art are omitted for the sake of clearness in understanding the concept of the invention, to avoid obscuring the invention with unnecessary detail.
(12) Disclosed herein is a solid-state avalanche radiation detector, and a method for constructing same, using amorphous material as the photoconductive layer without field hot-spots, to provide a direct conversion avalanche a-Se. The solid-state avalanche radiation detector is based on field-shaping by localizing the high-field avalanche region between two low-field regions, improving on the devices of Sauli, Lee, and Goldan. [9, 11, 14-16]
(13) The present disclosure optimizes the solid-state detector structure to provide stable avalanche multiplication gain in direct conversion amorphous selenium radiation detectors. The detector structure is referred to as a field-shaping multi-well avalanche detector (SWAD) that provides a practical manner to achieve stable avalanche in large area direct radiation detectors, by varying thickness of a low-field interaction region to stop high-energy radiation and optimizing the high-field multi-well detection region for avalanche multiplication.
(14) Stable avalanche multiplication gain is achieved by eliminating field hot-spots using high-density avalanche wells with insulated walls, with field-shaping within each well.
(15) The high-density insulated wells and field-shaping eliminates formation of field hot-spots in the avalanche region and eliminates high fields at the metal-semiconductor interface. The electric field at the metal-semiconductor interface is one order-of-magnitude lower than a peak value where avalanche occurs. The field-shaping electrodes, high-density insulated wells and field-shaping provide a semi-Gaussian field distribution inside each well.
(16)
(17)
(18)
(19)
(20) As shown in
(21)
(22) Dry etching may be performed using reactive ion etching (ME) or deep ME. Anisotropic etching of organic polymer dielectric is preferably performed with a deep ME tool using an inductively charged plasma (ICP) etch system at low pressure and low temperature. Anisotropic etching of oxide dielectrics, such as SiO, is preferably performed using fluorinated anisotropic etching where each dry etch sequence is followed by a secondary plasma deposition that furnishes a layer of fluorocarbon polymer passivation on the sidewalls. Other anisotropic etching techniques may be utilized as long as the oxide is only vertically etched at well bottoms without sidewall etching, thereby preserving oxide at the sidewalls during the etch to encapsulate the grid electrodes inside the wells.
(23)
(24)
(25)
(26)
(27)
(28)
(29) As shown in
(30)
(31)
(32)
(33)
(34) The etching of the well until the pixel electrode is preferably performed by: anisotropically etching the third dielectric layer 243 using oxygen plasma (02 plasma) inside an ICP deep ME system; etching the second conductive grid electrode layer 252 via dry etching of W with SF6 plasma; anisotropically etching the second dielectric layer using 02 plasma inside an ICP deep RIE system; etching the first conductive grid electrode layer via dry etching of W with SFG plasma; and anisotropically etching the first dielectric layer 241 using 02 plasma inside an ICP deep ME system.
(35) After etching the wells, SiO.sub.2 is conformally deposited using a TEOS-PECVD system, with
(36) As shown in
(37) The Cr mask is preferably etched using wet etching.
(38) As shown in
(39) Provided is a nanopattern, multi-well, solid-state a-Se radiation detector that includes a semiconductor, a pixel electrode, at least three dielectric layers, and at least two conductive grid electrode layers. The pixel electrode is deposited adjacent to the substrate and a first conductive grid electrode layer of the at least two conductive grid electrode layers is deposited on a first dielectric layer of the at least three dielectric layers. A second dielectric layer of the at least three dielectric layers is deposited on the first conductive grid electrode layer. A second conductive grid electrode layer of the at least two conductive grid electrode layers is deposited on the second dielectric layer. A third dielectric layer of the at least three dielectric layers is deposited on the second conductive grid electrode layer, and an etch mask is deposited on the third dielectric layer. A first etching forms at least two pillars with at least one well therebetween, an oxide dielectric layer is deposited on the at least two pillars and on a bottom of the at least one well, and a second etching removes the oxide dielectric layer from the bottom of the at least one well. More than two conductive grid electrode layers may also be utilized. If, e.g., three conductive grid electrode layers are utilized, a third dielectric layer is formed on the second conductive grid electrode layer, a third conductive grid electrode layer is formed on the third dielectric layer, and a fourth dielectric layer is formed on the third conductive grid electrode layer, thereby forming an n+1 dielectric layer on an nth conductive grid electrode layer, with the etch mask being deposited on the n+1 dielectric layer. The first etching is then performed to form at least two pillars with at least one well therebetween, as described above.
(40) The apparatus provided by the present disclosure provides a UTD charge sensing, which enables operating the detector at its theoretical limit of charge diffusion, improves in an avalanche-mode by more than three orders-of-magnitude.
(41) While the invention has been shown and described with reference to certain aspects thereof, it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the spirit and scope of the present invention as defined by the appended claims and equivalents thereof.
REFERENCES
(42) [1] J. A. Rowlands and S. Kasap; Amorphous Semiconductors Usher in Digital X-Ray Imaging. Phys. Today, 50(11):24-30, 1997. [2] N. F. Mott; Conduction in non-crystalline systems. VII. Non-ohmic behavior and switching. Phil. Mag., 24(190):911-934, 1971. [3] G. Juska and K. Arlauskas; Impact ionization and mobilities of charge carriers at high electric fields in amorphous selenium. Phys. Stat. Sol. (a), 59(0:389-393, 1980. [4] M. M. Wronski and J. A. Rowlands; Direct-conversion flat-panel imager with avalanche gain: Feasibility investigation for HARP-AMFPI. Medical Physics, 35(12):5207-5218, 2008. [5] M. M. Wronski, W. Zhao, A. Reznik, G. DeCrescenzo, K. Tanioka, and J. A. Rowlands; A solid-state amorphous selenium avalanche technology for low photon flux imaging applications. Med. Phys., 37(9):4982, 2010. [6] G. Juska, K. Arlauskas, J. Kocka, M. Hoheisel, and P. Chabloz; Hot Electrons in Amorphous Silicon. Physical Review Letters, 75:2984-2987, 1995. [7] K. Tanioka; The ultrasensitive TV pickup tube from conception to recent development. J. Mater. Sci.: Mater. Electron., 18(0):321-325, 2007. [8] U.S. Pat. No. 6,437,339 to Lee, et al., the content of which is incorporated herein by reference. [9] D. L. Y. Lee; Selenium detector with a grid for selenium charge gain. Proceedings of SPIE, 5745:216-222, 2005. [10] D. C. Hunt, K. Tanioka, and J. A. Rowlands. X-ray imaging using avalanche multiplication in amorphous selenium: Investigation of depth dependent avalanche noise. Med, Phys., 34(3):976-986, 2007. [11] U.S. Pat. No. 8,129,688 to A. H. Goldan, et al., the content of which is incorporated herein by reference. [12] A. H. Goldan, O. Tousignant, K. S. Karim, and J. A. Rowlands; Unipolar time-differential pulse response with a solid-state Charpak photoconductor. Appl. Phys. Lett., 101(21):213503, 2012. [13] A. H. Goldan, J. A. Rowlands, O. Tousignant, and K. S. Karim; Unipolar time-differential charge sensing in non-dispersive amorphous solids. J. Appl. Phys., 113(22):224502, 2013. [14] F. Sauli; GEM: A new concept for electron amplification in gas detectors. Nucl. Instr. and Meth. A, 386(2-3):531-534, 1997. [15] U.S. Pat. Publ. No. 2016/0087113 A1 of U.S. Appl. No. 14,888,879 to A. H. Goldan, et al., the content of which is incorporated herein by reference. [16] U.S. Pat. Publ. No. 2015/0171232 A1 of U.S. application Ser. No. 14/414,607 to A. H. Goldan, et al., the content of which is incorporated herein by reference. [17] A. H. Goldan, J. A. Rowlands, M. Lu, and W. Zhao; Nanopattern multi-well avalanche selenium detector with picosecond time resolution. In Proc. Conf. Rec. IEEE NSS/MIC, pages N32-4, Seattle, 2014.