CN103869237B - A kind of pulse laser number optimization method and the method for testing of SEU cross section - Google Patents

A kind of pulse laser number optimization method and the method for testing of SEU cross section Download PDF

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CN103869237B
CN103869237B CN201210536186.3A CN201210536186A CN103869237B CN 103869237 B CN103869237 B CN 103869237B CN 201210536186 A CN201210536186 A CN 201210536186A CN 103869237 B CN103869237 B CN 103869237B
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laser
section
cross
pulse laser
energy
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CN103869237A (en
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封国强
上官士鹏
韩建伟
马英起
余永涛
姜昱光
朱翔
陈睿
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National Space Science Center of CAS
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Abstract

The present invention relates to a kind of method optimizing pulse laser number, the method is for optimizing the pulse laser number of pulse laser test device SEU cross section, for a certain laser energy Ei, pulse laser number F uses following steps to determine: step 101) and obtain the facula area τ under this laser energy and device individual feature cellar area Δ;Step 102) obtain laser number judgement reference value, this judgement reference value is above-mentioned facula area τ and the ratio of device individual feature cellar area Δ;Step 103) when adjudicating reference value more than 1, described laser number determines according to facula area size;When adjudicating reference value less than 1, described laser number determines according to individual feature cellar area.When adjudicating reference value n more than 1, described laser number F=1/k τ;When n is less than 1, described laser number F=1/k Δ, wherein k is modulation factor, and its span is 1 25.

Description

A kind of pulse laser number optimization method and the method for testing of SEU cross section
Technical field
The invention mainly relates to a kind of new side utilizing pul sed laser simulation experimental test device SEU cross section Method, is that one is mainly directed towards the numeric class device SEU cross section tests such as memorizer, microprocessor and FPGA Test method, belong to spatial environments radiation effect ground simulation test technical field.
Background technology
In recent years, along with progressively reducing of semiconductor technology characteristic size, the numeral used in Chinese Space task Cmos device is the most gradually based on sub-micro device, and above-mentioned device is typically to play crucial work in electronic system The highly integrated chip such as microprocessor, FPGA and memorizer.Spoke when the high energy charged particles being in the outer space When penetrating in environment, occur Single event upset effecf cause the abnormal probability of chip operation with the reduction of process by Cumulative greatly.In view of highly integrated chip increase of direct application risk in space tasks, its anti-single particle is overturn The accurate evaluation of ability is that it is applied to the prerequisite of Spacecraft Electronic system.
Although high-energy particle accelerator is the best means carrying out device single particle effect test on ground, but due to examination The high cost tested and long period characteristic so that its application in terms of quick, low cost test receives limit greatly System.The pul sed laser simulation single particle effect examination grown up by United States Naval Research Laboratory from the eighties in last century Proved recipe method, because it is efficient, convenient and the feature such as low cost so that it is at single particle effect experimental test and study mechanism Aspect is widely used.Overseas utilization pulse laser research device single particle effect achieves a lot of achievement, Just deliver as far back as 1994 and utilized pulse laser to obtain SRAM SEU cross section σ~the article of E curve, Test data is provided for device radiation hardening.Domestic No.5 Academy, China Space Science and Technology Group Co., Ltd. the 510th grinds Study carefully institute, declared " experimental technique of a kind of pulsed laser single event upset cross section " in the end of the year 2011 (201010624396.9) patent, mainly on the basis of summing up the test method abroad delivered, proposes The method having test data support, to external published method without innovation, does not more account for device work The impact reducing pair cross-section test method of skill size.
And along with the reduction of device technology size, traditional SEU cross section test method, i.e. do not considering arteries and veins Under the influence of impulse light facula area size and device technology size relationship, the upset cross section result recorded and heavy ion Test data difference is the biggest.Therefore, the most simply according to the ratio relation of single-particle inversion number Yu pulse laser fluence Determine cross-section data, it is easy to produce owing to bigger facula area causes too much Multiple-bit upsets to cause cross section number According to bigger than normal, or same position is caused to be recovered the situation normally causing cross-section data less than normal by data after twice irradiation.This Test method consider process reduce on result of the test affect on the basis of, a kind of new section test is proposed Method so that the cross-section data of pulse laser test has preferable concordance with heavy ion result of the test.
Summary of the invention
It is an object of the invention to, in order to solve at the simple grain utilizing pulse laser test Super deep submicron process device During sub-upset cross section, the too much Multiple-bit upsets caused due to relatively large laser facula area or same position are by two Secondary irradiation upset number reduces, and the problem that the cross-section data that causes is bigger than normal or less than normal, thus propose a kind of pulse and swash Light number optimization method and the method for testing of SEU cross section.
To achieve these goals, the invention provides a kind of method optimizing pulse laser number, the method is used for Optimizing the pulse laser number of pulse laser test device SEU cross section, described method uses equation below to obtain Single event upset effecf cross section:
σ i = N F × M × S
Wherein, N is single-particle inversion number of times, and F is pulse laser number, and M is device storage position number, and S is The radiation exposed area of device, σiUpset cross section for i & lt test;
For a certain laser energy Ei, above-mentioned pulse laser number F uses following steps to determine:
Step 101) obtain the facula area τ under this laser energy and device individual feature cellar area Δ;
Step 102) obtain laser number judgement reference value, this judgement reference value is above-mentioned facula area τ and device list The ratio of individual functional unit area Δ;
Step 103) when adjudicating reference value more than 1, described laser number determines according to facula area size;When sentencing When certainly reference value is less than 1, described laser number determines according to individual feature cellar area.
Above-mentioned steps 103) particularly as follows:
When adjudicating reference value n more than 1, described laser number F=1/k τ;When n is less than 1, described laser Number F=1/k Δ, wherein k is modulation factor, and its span is 1-25.
Method based on above-mentioned optimization laser pulse number present invention also offers a kind of SEU cross section test side Method, described method comprises:
(1) tested device sample is chosen;
(2) being welded on pcb board by device example, described pcb board is fixed on an XY precision by switching Mobile station, and ensure that PCB moves with precision translation stages simultaneously;
(3) unbalanced pulse laser radiation source, sets laser scanning frequency, is focused selected laser also Determine the starting point that laser scans at device irradiation;
(4) the initial laser ENERGY E of test is chosen0, and the laser facula area after focusing on when recording this energy is big Little τ0, according to τ0Determine pulse laser number F with the size Δ of device example, add up single-particle inversion number N, according to Above-mentioned each parameter value obtains corresponding to ENERGY E0Upset cross section σ0
Continue to increase laser energy, until recording ENERGY E when device example upset cross section is not further added bys, and record Laser facula size τ after focusing on during this energys, according to τsPulse laser is determined with the size Δ of device example Number F, statistics single-particle inversion number N, maybe must correspond to ENERGY E according to above-mentioned each parameter value simultaneouslysTime upset Cross section σs;;
Finally, at above-mentioned E0To EsBetween when selecting the energy value of more than at least 3 to repeat each energy value of above-mentioned acquisition Upset cross section size;
(5) draw upset cross section σ~E curve according to the result of upper step, complete device in the case of different laser energy SEU cross section curve.
Also comprise after above-mentioned steps (5):
(6) close pulse laser single particle effect simulated test facility, and device is carried out power-off, turn off single-particle Upset effect test system;
(7) device SEU cross section will be obtained and σ~E curve will substitute into and estimates device in different track spaces Upset number of times software, assess the applicable orbit altitude of this device.
Above-mentioned steps (1) comprises further:
Sample is opened encapsulation process, and including front and Kaifeng, the back dress of device, device surface metal level is more than 3 The device of layer, only carries out Kaifeng, back;
After the dress of Kaifeng, unit for electrical property parameters and functional parameter to device are tested, and choose the device that can normally work Part sample is tested, and wherein for the print chosen with a device example no less than 3, and carries out print Numbering.
Also comprise between above-mentioned steps (3) and step (4):
After device has been placed, electricity on which, and utilize single-particle inversion test system to be electrically connected test, inspection Survey device and test system the most normally works;
After device and test system worked well, unbalanced pulse laser radiation source, set laser scanning frequency, right Selected laser is focused and determines the starting point that laser scans at device irradiation.
Compared with prior art, the invention have the benefit that
(1) upset cross section measured by laser is closer to heavy ion upset cross section;
(2) Multiple-bit upsets caused during the scanning of laser irradiation is decreased;
(3) it is that the anti-single particle upset ability of device is estimated and reinforcing provides data more accurately so that device It is more accurate to apply;
(4) laser energy is evenly distributed at device inside, it is to avoid the cross sectional testing uniformly caused because of laser energy is by mistake Difference.
Accompanying drawing explanation
Fig. 1 is pul sed laser simulation single particle effect test system used in the embodiment of the present invention 1;
Fig. 2 is that the hot spot after pulse laser focusing used in the embodiment of the present invention 1 is illustrated with the relation of energy variation Figure;
Fig. 3 be pulse laser focusing spot size used in the embodiment of the present invention 1 with device function cell size with And laser scanning location schematic diagram;
Fig. 4 is HM62V16100i conventional laser method of testing, the present invention test obtained in the embodiment of the present invention 1 σ~the E curve that method, heavy ion test method record.
Detailed description of the invention
Below in conjunction with the accompanying drawings present disclosure is described in further detail.
The process of a kind of novel combination device that the present invention provides and the test side of laser facula size Method so that the upset cross section data that laser is surveyed are more stable, closer to heavy ion data so that ground pulse laser The research of simulation SEU cross section is more reliable.
The invention aims to the single-particle solved utilizing pulse laser test Super deep submicron process device turn over When turning cross section, the too much Multiple-bit upsets caused due to relatively large laser facula area or same position are by two subradius Reduce according to upset number, and the problem that the cross-section data that causes is bigger than normal or less than normal.Propose a kind of novel combination device Process and the test method of laser facula size, overcome the test data that traditional method causes stable Property difference shortcoming.
Present invention is specific as follows:
Conventional test methods generally uses the mode of formula (1) to obtain Single event upset effecf cross section:
σ i = N F × M × S - - - ( 1 )
In formula, N be single-particle inversion number of times, F be pulse laser number, M be device storage position number unit bit, S is radiation exposed square measure cm of device2, σiUpset cross section unit cm for i & lt test2/bit。
Wherein the selection randomness of F is very big, is substantially determined by experimenter's subjectivity, and this is utilized pulse laser to obtain SEU cross section data bring the biggest uncertainty, are particularly reduced in size to ultra-deep Asia when device technology During micron, the selection of F is to σiImpact very big.
Therefore, the present invention proposes and utilizes the method for judgement reference value n i.e. formula (2) to determine laser number F:
N=τ/Δ (2)
In formula, τ is facula area size, and Δ is device individual feature cellar area size, and τ and Δ unit are all cm2
When n is more than 1, laser irradiation number of scan points, i.e. F=1/k τ to be determined according to facula area size;N is less than 1 Time, laser number F, i.e. F=1/k Δ to be determined according to device individual feature cellar area size;Wherein k is modulation The factor, span is between 1-25, and most preferably k value is 1.5.Require to arrange according to this, can be to greatest extent Utilize when reducing laser facula more than the size of one functional unit of device Multiple-bit upsets that laser irradiation causes and Test the situation that system statistics upset mistake is unstable under high-energy, and can guarantee that laser facula size is less than device During the size of one functional unit, irradiation is complete, obtains the device upset times N corresponding to laser energy E.
It is as follows that it is embodied as step:
(1) sample is opened encapsulation process before test, including front and Kaifeng, back dress, the device table of device The face metal level device more than 3 layers, can only carry out Kaifeng, back;After the dress of Kaifeng, be to the unit for electrical property parameters of device Testing with functional parameter, normal work just can be tested, and generally the print with a device is many In 3, and print is numbered;
(2) to be welded on by device as on its pcb board designed during test, PCB is fixed on one by switching XY precision translation stages, and ensure that PCB can move with mobile station simultaneously, device is placed on translation stage, Z axis Certain flatness is had at X/Y plane;
(3) after device has been placed, electricity on which, and it is utilized as the special single-particle inversion survey of this device design Test system is electrically connected test, and detection device and test system the most normally work;
(4) device and test system worked well after, unbalanced pulse laser radiation source, set laser scanning frequency, Selected laser is focused and determines the starting point that laser scans at device irradiation;
(5) the initial laser ENERGY E of test is chosen0, and the laser facula size after focusing on when recording this energy τ0, thereby determine that laser number F is tested, add up single-particle inversion number N, formula be calculated turning over of correspondence Turn cross section σ0
Repeat above-mentioned test procedure, continuing to increase laser energy, not being further added by i.e. turning over until recording device upset cross section Turning cross section saturated, corresponding laser energy is designated as Es, cross section is σs
Additionally, at E0To EsBetween select the cross-sectional sizes that the energy test of more than at least 3 is corresponding;
(6) according to testing different-energy, the laser SEU cross section of different fluence test chosen, just can obtain To device SEU cross section σ~E curve;
(7), after having tested, close pulse laser single particle effect simulated test facility, and device carried out power-off, Turn off Single event upset effecf test system.
(8) substitute into estimate device in different track spaces by obtaining device SEU cross section and σ~E curve The software of upset number of times, assesses the applicable orbit altitude of this device.
If it is required, multiple laser energy, laser fluence can be used, the most multiple laser fluences, repeat Above-mentioned steps (1)-(5) carry out irradiation scanning, record corresponding data, until it reaches test objective.
Embodiment
As a example by a 0.13 μm HM62V16100i SRAM, in conjunction with accompanying drawing to this test Method is described further.
Focusing unit 1-5 include 1-6 be colorful CCD camera, 1-7 be microscope, 1-8 be automatic focusing unit, 1-9 is automatic focusing objective len;1-14 measured device test control system include 1-10 be measured device, 1-11 be XY Translation stage, 1-12 be test pcb board (including device hardware test cell) used by device, 1-13 be observing and controlling meter Calculation machine.
Concrete annexation is as follows:
Annexation: wherein, 1-1 is that (laser pulse width is adjustable, and scope is femtosecond fs, psec ps for pulse laser And nanosecond ns magnitude), 1-2 be laser energy regulation unit, 1-3 be laser energy beam splitting arrangement, 1-4 be laser Energy meter, 1-5 autofocus system, 1-6 be colorful CCD camera, 1-7 be that microscope, 1-8 are for automatically focusing on Unit, 1-9 be automatic focusing objective len, 1-10 be measured device, 1-11 be XY translation stage, 1-12 be test device Pcb board (including device hardware test cell), 1-13 used are Measurement &control computer, and 1-14 is that measured device is surveyed Examination control system.
Embodiment 1
Pul sed laser simulation HM62V16100i Single event upset effecf test, its pilot system figure as shown in Figure 1: 1-1 is pulse laser (laser pulse width is adjustable, scope is femtosecond fs, psec ps and nanosecond ns magnitude), 1-2 Regulate unit for laser energy, 1-3 is laser energy beam splitting arrangement, 1-4 is that laser energy meter, 1-5 focus on system automatically System, 1-6 be colorful CCD camera, 1-7 be microscope, 1-8 be automatic focusing unit, 1-9 be automatic conglomeration Mirror, 1-10 be measured device, 1-11 be XY translation stage, 1-12 be that test pcb board used by device (includes device Part hardware testing unit), 1-13 be Measurement &control computer, 1-14 is measured device test control system;2-1 is laser Energy (nJ), 2-2 are laser spot diameter (μm); 3-1 be Chip-wide, 3-2 be laser facula, one functional unit width Delta of 3-3 chipx, 3-4 be one merit of chip Can element length Δy, 3-5 be spot diameter;4-1 is laser energy (nJ), 4-2 conventional laser method of testing is surveyed σ~E cross section curve, 4-3 are surveyed σ~E cross section curve by heavy ion, 4-4 is surveyed σ~E cross section song by the present invention Line, 4-5 are upset cross section value (unit (cm2/bit)。
Measurement σ~E using above-mentioned component units to provide overturns curved section method particularly includes:
(1) HM62V16100i is opened back encapsulation process and carries out unit for electrical property parameters and functional parameter is carried out Test, normal work just can be tested, and selects 3 pieces of prints, numbering 1,2,3;
(2) to select the device of numbered 1 to be welded on as on its pcb board designed during test, PCB is by turning Connect and be fixed on an XY three-dimensional precise mobile station (precision is up to 0.1 μm~1 μm), and ensure PCB and mobile station Can move simultaneously, and pcb board is connected with Measurement &control computer.Device is placed on translation stage, and Z axis is put down at XY There is certain flatness in face, utilizes Measurement &control computer to implement monitoring laser focusing on device back silicon substrate, Automatically focusing unit makes laser in device surface difference in height less than 5 μm, reaches this and requires that guarantee laser hangs down During straight irradiation, energy is evenly distributed at device inside;
(3) determine irradiation scan start point, according to the fluence of heavy ion, arrange laser fluence (parameter include X, Y-axis translational speed, laser frequency), utilize the primary power of 1nJ that the device of normal work is tested, until Record device turn threshold ENERGY E0With upset number and saturated upset cross section inversion energy EsWith upset number;
(4) E is selected after completing0、Es、E0And EsBetween 3 energy, 5 energy values altogether, test hot spot The relation such as table 1 of diameter, the spot diameter size recorded and energy, draw to obtain Fig. 2;
Table 1 spot diameter size and the relation of energy
(5) big with the individual feature cellar area of device by the selected laser facula size for 5 energy of test Little ratio, such as Fig. 3, determines the relation such as table 2 of laser fluence, laser fluence and energy;
Table 2 laser fluence and energy relationship
Laser energy (nJ) Laser fluence (cm-2)
5 6.3×106
10 4×106
15 2.8×106
20 2.8×106
30 2.8×106
(6) 5 upset cross section recorded the results are shown in Table 3, and laser single-particle σ~E overturns curved section such as Fig. 4. In order to contrast, putting in table 3 by heavy ion, conventional laser method of testing surveyed cross section result, σ~E overturns curve Cross section is put in the diagram;
Table 3 distinct methods records HM62V16100i upset cross section test result
(7), after having tested, close pulse laser single particle effect simulated test facility, and device carried out power-off, Turn off Single event upset effecf test system;
(8) device SEU cross section will be obtained and σ~E curve will substitute into and estimates device at different track spaces In upset number of times software, assess the applicable orbit altitude of this device.
It should be noted that the embodiment of present invention described above and and unrestricted.Those skilled in the art Should be appreciated that any technical solution of the present invention is revised or be equal to replacement without departure from technical solution of the present invention Spirit and scope, it all should be contained in scope of the presently claimed invention.

Claims (6)

1. the method optimizing pulse laser number, the method is used for optimizing pulse laser test device single-particle The pulse laser number of upset cross section, described method comprises the steps of;
For a certain laser energy Ei, pulse laser number F of optimization uses following steps to determine:
Step 101) obtain the facula area τ under this laser energy and device individual feature cellar area Δ;
Step 102) obtain laser number judgement reference value, this judgement reference value is above-mentioned facula area τ and device list The ratio of individual functional unit area Δ;
Step 103) when adjudicating reference value more than 1, described laser number determines according to facula area size;When sentencing When certainly reference value is less than 1, described laser number determines according to individual feature cellar area;
Described step 103) particularly as follows:
When adjudicating reference value n more than 1, described laser number F=1/k τ;When n is less than 1, described laser Number F=1/k Δ, wherein k is modulation factor, and its span is 1-25.
2. the SEU cross section test side of the method optimizing pulse laser number according to claim 1 Method, it is characterised in that described SEU cross section method of testing uses equation below to obtain Single event upset effecf Cross section:
σ i = N F × M × S
Wherein, N is single-particle inversion number of times, and F is to optimize the pulse laser number obtained, and M is that device stores position Number, S is the radiation exposed area of device, σiUpset cross section for i & lt test.
The SEU cross section method of testing of the method for optimization pulse laser number the most according to claim 2, It is characterized in that, described SEU cross section method of testing specifically comprises the steps of:
(1) tested device sample is chosen;
(2) being welded on pcb board by device example, described pcb board is fixed on an XY precision by switching Mobile station, and ensure that PCB moves with precision translation stages simultaneously;
(3) unbalanced pulse laser radiation source, sets laser scanning frequency, is focused selected laser also Determine the starting point that laser scans at device irradiation;
(4) the initial laser ENERGY E of test is chosen0, and the laser facula area after focusing on when recording this energy is big Little τ0, according to τ0Determine pulse laser number F with the size Δ of device example, add up single-particle inversion number N, according to Above-mentioned parameter τ0, F and N value obtain corresponding to ENERGY E0Upset cross section σ0
Continue to increase laser energy, until recording ENERGY E when device example upset cross section is not further added bys, and record Laser facula size τ after focusing on during this energys, according to τsPulse laser is determined with the size Δ of device example Number F, simultaneously statistics single-particle inversion number N, according to above-mentioned parameter τ0, F and N value obtain corresponding to ENERGY EsTime Upset cross section σs
Finally, at above-mentioned E0To EsBetween turning over when selecting the energy value of at least 3 to repeat each energy value of above-mentioned acquisition Turn cross-sectional sizes;
(5) draw upset cross section σ~E curve according to the result of upper step, complete device in the case of different laser energy SEU cross section curve.
The SEU cross section method of testing of the method for optimization pulse laser number the most according to claim 3, It is characterized in that, also comprise after described step (5):
(6) close pulse laser single particle effect simulated test facility, and device is carried out power-off, turn off single-particle Upset effect test system;
(7) device SEU cross section will be obtained and σ~E curve will substitute into and estimates device in different track spaces Upset number of times software, assess the applicable orbit altitude of this device.
The SEU cross section method of testing of the method for optimization pulse laser number the most according to claim 3, It is characterized in that, described step (1) comprises further:
Sample is opened encapsulation process, and including front and Kaifeng, the back dress of device, device surface metal level is more than 3 The device of layer, only carries out Kaifeng, back;
After the dress of Kaifeng, unit for electrical property parameters and functional parameter to device are tested, and choose the device that can normally work Part sample is tested, and wherein for the print chosen with a device example no less than 3, and carries out print Numbering.
The SEU cross section test side of the method for optimization pulse laser number the most according to claim 5 Method, it is characterised in that also comprise between described step (2) and step (3):
After device has been placed, electricity on which, and utilize single-particle inversion test system to be electrically connected test, inspection Survey device and test system the most normally works.
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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105022859B (en) * 2015-05-08 2018-01-19 西北核技术研究所 A kind of quantitative analysis method of the heavy ion single event multiple bit upset effect of device
CN105445640B (en) * 2015-11-24 2018-05-08 北京时代民芯科技有限公司 The single-particle sensitiveness decision method of different instruction set based on pulse laser equipment
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CN105510809B (en) * 2016-01-26 2018-07-20 工业和信息化部电子第五研究所 Pul sed laser simulation single particle experiment system and method
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CN109509507B (en) * 2018-11-02 2021-01-05 中国科学院上海微系统与信息技术研究所 Test circuit, test system and method for single event upset of SRAM (static random Access memory) storage unit
CN111486949B (en) * 2020-04-13 2021-06-22 中国科学院西安光学精密机械研究所 Transient M2Factor measuring instrument

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101561477A (en) * 2009-05-15 2009-10-21 中国人民解放军国防科学技术大学 Method and device for testing single event upset in in-field programmable logic gate array
CN102169022A (en) * 2010-12-31 2011-08-31 中国航天科技集团公司第五研究院第五一○研究所 Experiment method for pulsed laser single event upset cross section
CN102495355A (en) * 2011-12-31 2012-06-13 中国科学院微电子研究所 Laser pulse single particle effect simulation system

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3887365B2 (en) * 2003-09-22 2007-02-28 富士通株式会社 Radiation electromagnetic field tolerance calculation device and program recording medium
US7023235B2 (en) * 2003-12-12 2006-04-04 Universities Research Association, Inc. Redundant single event upset supression system

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101561477A (en) * 2009-05-15 2009-10-21 中国人民解放军国防科学技术大学 Method and device for testing single event upset in in-field programmable logic gate array
CN102169022A (en) * 2010-12-31 2011-08-31 中国航天科技集团公司第五研究院第五一○研究所 Experiment method for pulsed laser single event upset cross section
CN102495355A (en) * 2011-12-31 2012-06-13 中国科学院微电子研究所 Laser pulse single particle effect simulation system

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
利用脉冲激光开展的卫星用器件和电路单粒子效应试验;韩建伟 等;《航天器环境工程》;20090430;第26卷(第2期);第125-130页 *
深亚微米SRAM器件单粒子效应的脉冲激光辐照试验研究;上官士鹏 等;《原子能科学技术》;20120831;第46卷(第8期);第1019-1024页 *

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