IP Library Granted Patent US 12,070,819
Granted Patent B2
US 12,070,819 · App. 17/272,155 · Granted Aug 27, 2024

Systems and methods for drilling vias in transparent materials

Inventors: Hisashi Matsumoto (Portland, OR); Jan Kleinert (Portland, OR); Zhibin Lin (Portland, OR)
Assignee: ELECTRO SCIENTIFIC INDUSTRIES, INC.
B23K26/382B23K26/0624B23K26/402B23K2103/50
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Quick Facts
Patent No.
US 12,070,819
App. No.
17/272,155
Granted
Aug 27, 2024
Kind
B2
Abstract

A method for forming a through-via in a substrate having opposing first and second surfaces can include directing a focused beam of laser pulses into the substrate through the first surface of the substrate and, subsequently, through the second surface of the substrate. The focused beam of laser pulses can have a wavelength to which the substrate is at least substantially transparent and a beam waist of the focused beam of laser pulses is closer to the second surface than to the first surface. The focused beam of laser pulses is characterized by a pulse repetition rate, a peak optical intensity at the substrate and an average power at the substrate sufficient to: melt a region of the substrate near the second surface, thereby creating a melt zone within the substrate; propagate the melt zone toward the first surface; and vaporize or boil material of the substrate and located within the melt zone.

Claims (41)

1. A method for forming a through-via in a substrate, the method comprising:

providing a substrate having a first surface and a second surface opposite the first surface; and

directing, during a drilling period less having a duration less than 100 μs, a focused beam of laser pulses into the substrate at a location through the first surface of the substrate and, subsequently, through the second surface of the substrate,

wherein the focused beam of laser pulses has a wavelength to which the substrate is at least substantially transparent,

wherein an optical intensity of the focused beam of laser pulses at the substrate is less than an optical breakdown intensity of the substrate,

wherein the focused beam of laser pulses has a Gaussian energy distribution,

wherein the focused beam of laser pulses has a pulse repetition rate greater than 5 MHz, and

wherein laser pulses within the focused beam of laser pulses have a pulse width greater than 200 fs.

2. The method of claim 1 , wherein the substrate is at least substantially transparent to at least one wavelength in the ultraviolet, visible or infrared regions of the electromagnetic spectrum.

3. The method of claim 2 , wherein the substrate is at least substantially transparent to at least one wavelength in the visible region of the electromagnetic spectrum.

4. The method of claim 2 , wherein the substrate is at least substantially transparent to at least one wavelength in the infrared region of the electromagnetic spectrum.

5. The method of claim 1 , wherein the substrate is glass.

6. The method of claim 1 , wherein the substrate is sapphire.

7. The method of claim 1 , wherein the substrate is a silicon die.

8. The method of claim 1 , wherein the substrate is a GaN die.

9. The method of claim 1 , wherein the focused beam of laser pulses has a pulse repetition rate greater than 25 MHz.

10. The method of claim 9 , wherein the focused beam of laser pulses has a pulse repetition rate greater than 40 MHz.

11. The method of claim 10 , wherein the focused beam of laser pulses has a pulse repetition rate greater than 300 MHz.

12. The method of claim 11 , wherein the focused beam of laser pulses has a pulse repetition rate greater than 500 MHz.

13. The method of claim 10 , wherein laser pulses within the focused beam of laser pulses have a pulse width less than 50 ps.

14. A method for forming a through-via in a substrate, the method comprising:

providing a substrate having a thickness in a range from 30 μm to 150 μm and having a first surface and a second surface opposite the first surface; and

directing a focused beam of laser pulses into the substrate through the first surface of the substrate and, subsequently, through the second surface of the substrate,

wherein the focused beam of laser pulses has a wavelength to which the substrate is at least substantially transparent;

wherein an optical intensity of the focused beam of laser pulses at the substrate is less than an optical breakdown intensity of the substrate;

wherein the focused beam of laser pulses has a Gaussian energy distribution;

wherein the focused beam of laser pulses has a pulse repetition rate, a peak optical intensity at the substrate and an average power at the substrate driving a cumulative heating effect to melt a region of the substrate irradiated by the focused beam of laser pulses; and

wherein laser pulses within the focused beam of laser pulses have a pulse width,

wherein the peak optical intensity, pulse repetition rate, average power and pulse width are selected such that the through-via is formed in less than 40 μs.

15. The method of claim 14 , wherein the peak optical intensity, pulse repetition rate, average power and pulse width are selected such that the through-via is formed in less than 30 μs.

16. The method of claim 15 , wherein the peak optical intensity, pulse repetition rate, average power and pulse width are selected such that the through-via is formed in less than 20 μs.

17. The method of claim 16 , wherein the peak optical intensity, pulse repetition rate, average power and pulse width are selected such that the through-via is formed in less than 10 μs.

18. The method of claim 15 , wherein the peak optical intensity, pulse repetition rate, average power and pulse width are selected such that the through-via is formed in a range from 5 μs to 15 μs.

19. A method for forming a through-via in a substrate, the method comprising:

providing a substrate having a first surface and a second surface opposite the first surface; and

directing a focused beam of laser pulses into the substrate through the first surface of the substrate and, subsequently, through the second surface of the substrate,

wherein the focused beam of laser pulses has a wavelength to which the substrate is at least substantially transparent and wherein a beam waist of the focused beam of laser pulses is located within the substrate closer to the second surface of the substrate than to the first surface of the substrate, and

wherein the focused beam of laser pulses is characterized by a pulse repetition rate, a peak optical intensity at the substrate and an average power at the substrate sufficient to:

melt a region of the substrate near the second surface, thereby creating a melt zone within the substrate;

propagate the melt zone toward the first surface; and

vaporize or boil material of the substrate located within the melt zone.

Assignments (6)
RELEASE OF SECURITY INTEREST Recorded Aug 24, 2022
From: BARCLAYS BANK PLC
To: MKS INSTRUMENTS, INC.; NEWPORT CORPORATION; ELECTRO SCIENTIFIC INDUSTRIES, INC.
Reel/Frame 062739/0001 →
RELEASE OF SECURITY INTEREST Recorded Aug 24, 2022
From: BARCLAYS BANK PLC
To: MKS INSTRUMENTS, INC.; NEWPORT CORPORATION; ELECTRO SCIENTIFIC INDUSTRIES, INC.
Reel/Frame 063009/0001 →
SECURITY INTEREST Recorded Aug 19, 2022
From: MKS INSTRUMENTS, INC.; NEWPORT CORPORATION; ELECTRO SCIENTIFIC INDUSTRIES, INC.
To: JPMORGAN CHASE BANK, N.A., AS COLLATERAL AGENT
Reel/Frame 061572/0069 →
PATENT SECURITY AGREEMENT (TERM LOAN) Recorded Apr 29, 2021
From: ELECTRO SCIENTIFIC INDUSTRIES, INC.; NEWPORT CORPORATION; MKS INSTRUMENTS, INC.
To: BARCLAYS BANK PLC
Reel/Frame 056101/0652 →
PATENT SECURITY AGREEMENT (ABL) Recorded Apr 29, 2021
From: ELECTRO SCIENTIFIC INDUSTRIES, INC.; MKS INSTRUMENTS, INC.; NEWPORT CORPORATION
To: BARCLAYS BANK PLC
Reel/Frame 056101/0783 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 26, 2021
From: MATSUMOTO, HISASHI; KLEINERT, JAN; LIN, ZHIBIN
To: ELECTRO SCIENTIFIC INDUSTRIES, INC.
Reel/Frame 055433/0423 →