IP Library › Granted Patent US 12,332,187
Granted Patent B2
US 12,332,187 · App. 18/249,454 · Granted Jun 17, 2025

Photoluminescence measurement device

Inventors: Renaud Varache (Grenoble, FR); Patrick Jeremy Dahan (Paris, FR)
Assignee: COMMISSARIAT A L'ENERGIE ATOMIQUE ET AUX ENERGIES ALTERNATIVES
G01N21/9505G01N21/6489G01N21/956H02S50/15G01N2021/646G01N2021/8461
View Patent ↗
Loading inventors, assignments & file history…
Monitor This Case
Get email alerts when status or documents change.
Order Certified Copies
Most orders are placed with the USPTO same day — all within 24 business hours.
Order via The Patent Place →
Pre-filled with this patent's details
Quick Facts
Patent No.
US 12,332,187
App. No.
18/249,454
Granted
Jun 17, 2025
Kind
B2
Abstract

A photoluminescence measurement device may include: a sample holder; a detector configured to collect a photoluminescence signal; a processing unit configured to process a signal collected by the detector; and a support disposed facing a rear face of the sample holder, opposite to the front face, and on one face, called the main face, of which rests at least one radiation source for emitting light radiation illuminating the rear face and likely to be collected, by transparency of the sample holder with respect to the light radiation, by the detector.

Claims (56)

1. A photoluminescence or electroluminescence measurement device, comprising:

a sample holder;

a detector configured to collect a photoluminescence or electroluminescence signal emitted by a sample likely to be disposed on a front face of the sample holder;

a processing unit configured to process a signal collected by the detector; and

a support disposed facing a rear face of the sample holder, opposite to the front face, and on a main face, of which at least one radiation source rests for emitting light radiation illuminating the rear face and likely to be collected, by transparency of the sample holder with respect to the light radiation, by the detector,

wherein, when a sample having a contour C rests through a first face on the front face of the sample holder, and so that the sample is circumscribed by an overflow zone of the sample holder, through which light radiation, likely to be emitted by the at least one radiation source, is likely to pass, and

wherein the detector is also configured to establish mapping of light intensity of the radiation likely to pass through the overflow zone and of the photoluminescence signal emitted by the sample.

2. The device of claim 1 , wherein the at least one radiation source comprises a plurality of radiation sources arranged in a matrix form on the main face.

3. The device of claim 2 , further comprising a diffuser interposed between the sample holder and the support, and

wherein the diffuser is configured to homogenize light radiation likely to be emitted by the radiation sources.

4. The device of claim 3 , wherein the sample holder, the diffuser, and the support are held integral with each other by a holder.

5. The device of claim 4 , further comprising:

a filter configured to filter in wavelength light radiation likely to be emitted by the radiation sources.

6. The device of claim 3 , further comprising:

a filter configured to filter in wavelength light radiation likely to be emitted by the radiation sources.

7. The device of claim 1 , wherein the processing unit comprises a computer program designed to implement a process comprising:

(a) extracting a light intensity profile along a linear trace overlapping the contour of the sample, the profile comprising a first section associated with the intensity of the light radiation passing through the overflow zone, and a second section associated with the intensity of the photoluminescence of the electroluminescence emitted by the sample;

(b) determining the position x o , associated with an intensity y o of the signal, and tracked from a reference position of the first section, of the contour on the light intensity profile, the determining comprising a slope calculation, the position x o corresponding to a position for which a break of slope greater in absolute value than a predetermined value is observed in a direction from the first section to the second section, the predetermined value advantageously being greater than 10%.

8. The device of claim 7 , wherein the computer program is further designed to implement:

(c) determining a reference intensity y max in the second section S 2 , said reference intensity y max corresponding to a sliding maximum;

(d) determining a first extent E 1 according to a so-called tangent method, the tangent method comprising:

(d1) calculating the slope P o of a straight line D o passing through the point of coordinates x o and y o and through another point of the edge of the sample taken on the linear trace;

(d2) calculating a position, called target position x c , for which the straight line D o has an ordinate equal to 70% of the deviation between the reference intensity y max and the intensity y o ;

(d3) calculating a deviation between the target position x c and the position x o , the deviation being associated with the first extent E 1 ;

(e) determining a second extent E 2 according to a so-called direct method, the direct method comprising:

(e1) determining a direct position x d , for which the intensity, in the second section S 2 , is equal to 70% of the deviation between the reference intensity y max and the intensity y o ;

(e2) calculating a deviation between the direct position x d and the position x o , the deviation being associated with the second extent E 2 ; and

(f) calculating an edge width D so defined as the minimum value between the first extent E 1 and the second extent E 2 .

9. The device of claim 7 , wherein the predetermined value is greater than 10%.

10. The device of claim 8 , wherein the computer program is also designed to calculate a metric M representative of the amount of defects present at the edge of plates,

wherein the metric M satisfies equation (I):

M

=

∫

x

o

D

y

max

-

y

(

x

)

y

max

⁢

dx

,

(

I

)

wherein y(x) represents a intensity profile variation along the linear trace as a function of its position x.

11. The device of claim 1 , further comprising:

a light emission source configured for inducing emission of a photoluminescence signal by a sample likely to rest on the front face of the sample holder.

12. The device of claim 11 , wherein the detector is configured to collect the photoluminescence signal.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jun 26, 2023
From: VARACHE, RENAUD; DAHAN, PATRICK JEREMY
To: COMMISSARIAT A L'ENERGIE ATOMIQUE ET AUX ENERGIES ALTERNATIVES
Reel/Frame 064054/0090 →
Priority Claims (1)
FR 2010774 · Oct 21, 2020 · national
Continuity (1)
Related Publication 20230400418A1 · Dec 14, 2023
References Cited (9)
US 5741171A · Sarfaty · 1998 [cited by examiner]
US 8269830B1 · Delaney · 2012 [cited by applicant]
US 10672119B2 · Yamaguchi · 2020 [cited by examiner]
US 20060029284A1 · Stewart · 2006 [cited by applicant]
WO WO2019117228A1 · 2019 [cited by applicant]
International Search Report and Written Opinion issued Jan. 31, 2022 in PCT/FR2021/051831 filed on Oct. 20, 2021 21 pages. [cited by applicant]
Song, Mei-Ping et al. “Research on Broken Corner and Black Edge Detection of Solar Cell” Proceedings of the 2018 International Conference on Machine Learning and Cybernetics (ICMLC), IEEE, vol. 1, Jul. 15, 2018, pp. 80-… [cited by applicant]
Williams, D.J. et al. “Normalized edge detector” Proceedings of the International Conference on Pattern Recognition. Atlantic City, Jun. 16-21, 1990. Conference A: Computer Vision and Conference B: Pattern Recognition S… [cited by applicant]
Bao-Shan, Shi et al. “A Method for Threshold Selection in Edge Width Detection of Objects in the Image” 2009 International Conference on Signal Processing Systems, IEEE May 15, 2009. pp. 402-405 (4 pages). [cited by applicant]