EP0075709B1 - Spektrometer zum Nachweis der von einer Elektronensonde auf einer Probe ausgelösten Sekundärelektronen - Google Patents
Spektrometer zum Nachweis der von einer Elektronensonde auf einer Probe ausgelösten Sekundärelektronen Download PDFInfo
- Publication number
- EP0075709B1 EP0075709B1 EP82107490A EP82107490A EP0075709B1 EP 0075709 B1 EP0075709 B1 EP 0075709B1 EP 82107490 A EP82107490 A EP 82107490A EP 82107490 A EP82107490 A EP 82107490A EP 0075709 B1 EP0075709 B1 EP 0075709B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- secondary electrons
- spectrometer
- electrode
- target
- potential
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 239000000523 sample Substances 0.000 title claims description 22
- 238000005259 measurement Methods 0.000 description 6
- 238000010894 electron beam technology Methods 0.000 description 3
- 230000001960 triggered effect Effects 0.000 description 3
- 230000001133 acceleration Effects 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J49/00—Particle spectrometers or separator tubes
- H01J49/02—Details
- H01J49/08—Electron sources, e.g. for generating photo-electrons, secondary electrons or Auger electrons
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J49/00—Particle spectrometers or separator tubes
- H01J49/44—Energy spectrometers, e.g. alpha-, beta-spectrometers
Definitions
- the invention relates to a spectrometer for detecting the secondary electrons triggered by an electron probe on a sample according to the preamble of claim 1.
- the potential measurement on a sample with an electron probe requires a spectrometer, which is used to measure the secondary electron energy.
- the spectrometer arrangement previously used is described in the literature (H.P. Feuerbaum, "VLSI Testing Using The Electron Probe", SEM / 1979, SEM Inc.AMF O'HARE IL 60666, 285-296).
- the secondary electrons released on the sample pass through a suction field and are then braked in a homogeneous opposing field.
- This known counterfield spectrometer delivers an integral energy distribution.
- the angular distribution of the secondary electrons is not taken into account.
- this angular distribution can be changed by electrostatic micro-fields on the sample surface, i.e. If the potential at the measuring point changes, so does the local microfield on the sample surface and thus also the angular distribution of the secondary electrons. Since the secondary electron spectrometer does not see the change in the angular distribution of the secondary electrons, measurement errors of approximately 5-10% occur in the known arrangement.
- the present invention is based on the object of specifying a secondary electron spectrometer of the type mentioned at the outset which is improved in terms of measuring accuracy.
- the measurement sensitivity is also improved with a secondary electron spectrometer arrangement according to the invention.
- the figure shows a secondary electron spectrometer arrangement according to the invention.
- the secondary electron spectrometer shown in the figure was designed in order to significantly increase the detection probability for the secondary electrons emitted at larger angles relative to the primary beam axis compared to arrangements with planar counterfield electrodes.
- the improvement according to the invention can therefore advantageously be carried out on a secondary electron spectrometer of an electron beam measuring device, as described in the publication by H.P. Feuerbaum is known.
- the secondary electrons are extracted from the sample by a suction field AI of high field strength. This suction field A1 is located between the grid G1 and the sample PR.
- the measuring points on the sample PR are usually in the non-activated state at the potential 0, while, as is also known from the cited literature reference, the grid G1 is at a high potential, e.g. B. 600 V. After passing through the suction field A1, the secondary electrons pass through a braking opposing field BF between the two grids G1 and G2. As is also known from the cited literature reference, the grid G2 is again at approximately the same potential as the measuring points on the sample PR in the non-activated state.
- the braking opposing field BF between the grids G1 and G2 is such that it only cancels the previous acceleration of the suction field A1. All secondary electrons SE can thus pass through the grid G2 and then have an angular distribution which is identical to the angular distribution of the secondary electrons SE on the sample surface.
- the energy distribution of the secondary electrons SE is then measured using the hemispherical grid G3, which is at a potential of approximately -7 V in the exemplary embodiment shown in the figure.
- the secondary electrons SE in the suction field A2 are then accelerated to the detector via a further grid arrangement G4.
- the grid arrangement G4 is operated at approximately the same voltage as in the secondary electron spectrometer described in the cited reference.
- the secondary electron spectrometer is also provided with an AB shield.
- the primary electron beam PE impinges on the sample PR and generates secondary electrons SE with a certain angular distribution that depends on the potential at the measuring point on the sample surface.
- the invention is particularly suitable for the quantitative potential measurement on integrated circuits with an electron probe.
- the invention it is essential for the invention to project the angular distribution of the secondary electrons SE present on the sample surface, which depends on the potential of the measuring point on the sample surface, onto the plane of the grid G2, the secondary electrons SE essentially have the same three-dimensional pulse distribution as at the measuring point on the sample surface at the time of generation of the secondary electrons SE by the primary electron beam PE. It is also essential for the invention that the secondary electrons SE accelerate with this three-dimensional pulse distribution after passing through the grid G2 be that a change in the angular distribution due to a change in potential at the measuring point on the sample surface does not falsify the measurement of the energy distribution of the secondary electrons SE in the detector.
- the secondary electrons SE are braked.
- the voltage of approximately -7 V applied to the grid G3 is selected such that secondary electrons SE, which are triggered at measuring points (conductor tracks) to which a voltage of approximately 8 V is applied, are just triggered into the suction field A2 of the grid arrangement G4 and finally can get to the detector.
- the invention is of course not limited to the embodiment shown in the figure.
- the effects of the grids G1, G2, G3 can also be achieved by only two grids shaped in a certain way, the first grille being designed as a suction grille and the second grille as a brake grille.
Landscapes
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
- Testing Or Measuring Of Semiconductors Or The Like (AREA)
- Electron Tubes For Measurement (AREA)
- Testing Of Individual Semiconductor Devices (AREA)
- Tests Of Electronic Circuits (AREA)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE3138929 | 1981-09-30 | ||
DE19813138929 DE3138929A1 (de) | 1981-09-30 | 1981-09-30 | Verbessertes sekundaerelektronen-spektrometer fuer die potentialmessung an einer probe mit einer elektronensonde |
Publications (3)
Publication Number | Publication Date |
---|---|
EP0075709A2 EP0075709A2 (de) | 1983-04-06 |
EP0075709A3 EP0075709A3 (en) | 1983-06-29 |
EP0075709B1 true EP0075709B1 (de) | 1987-04-08 |
Family
ID=6143065
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP82107490A Expired EP0075709B1 (de) | 1981-09-30 | 1982-08-17 | Spektrometer zum Nachweis der von einer Elektronensonde auf einer Probe ausgelösten Sekundärelektronen |
Country Status (4)
Country | Link |
---|---|
US (1) | US4514682A (enrdf_load_stackoverflow) |
EP (1) | EP0075709B1 (enrdf_load_stackoverflow) |
JP (1) | JPS5871542A (enrdf_load_stackoverflow) |
DE (2) | DE3138929A1 (enrdf_load_stackoverflow) |
Families Citing this family (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS59211953A (ja) * | 1983-05-17 | 1984-11-30 | Univ Osaka | 2次電子分光装置 |
GB8327737D0 (en) * | 1983-10-17 | 1983-11-16 | Texas Instruments Ltd | Electron detector |
DE3638682A1 (de) * | 1986-11-13 | 1988-05-19 | Siemens Ag | Spektrometerobjektiv fuer korpuskularstrahlmesstechnik |
JPS63126148A (ja) * | 1986-11-14 | 1988-05-30 | Hiroshi Daimon | 荷電粒子アナライザ− |
JP2696216B2 (ja) * | 1988-01-11 | 1998-01-14 | セイコーインスツルメンツ株式会社 | イオンビーム加工装置 |
JPH03101041A (ja) * | 1989-09-14 | 1991-04-25 | Hitachi Ltd | 電子ビームによる電圧測定装置 |
US6359451B1 (en) | 2000-02-11 | 2002-03-19 | Image Graphics Incorporated | System for contactless testing of printed circuit boards |
AU3354401A (en) | 2000-02-14 | 2001-08-20 | Eco 3 Max Inc. | Process for removing volatile organic compounds from an air stream and apparatustherefor |
RU2171467C1 (ru) * | 2000-06-30 | 2001-07-27 | Санкт-Петербургский государственный электротехнический университет | Микрореактор для химического и генетического тестирования |
WO2016047538A1 (ja) * | 2014-09-24 | 2016-03-31 | 国立研究開発法人物質・材料研究機構 | エネルギー弁別電子検出器及びそれを用いた走査電子顕微鏡 |
US10319578B2 (en) * | 2016-01-21 | 2019-06-11 | Japan Synchrotron Radiation Research Institute | Retarding potential type energy analyzer |
Family Cites Families (15)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2946002A (en) * | 1958-02-17 | 1960-07-19 | Kingston Electronic Corp | Signal-pickup test probe |
US3445708A (en) * | 1967-02-06 | 1969-05-20 | Gen Electric | Electron diffraction unit |
US3531716A (en) * | 1967-06-16 | 1970-09-29 | Agency Ind Science Techn | Method of testing an electronic device by use of an electron beam |
US3448377A (en) * | 1967-10-12 | 1969-06-03 | Atomic Energy Commission | Method utilizing an electron beam for nondestructively measuring the dielectric properties of a sample |
US3549999A (en) * | 1968-06-05 | 1970-12-22 | Gen Electric | Method and apparatus for testing circuits by measuring secondary emission electrons generated by electron beam bombardment of the pulsed circuit |
DE1946931A1 (de) * | 1969-09-17 | 1971-03-18 | Gen Electric | Verfahren zum Pruefen von Schaltungen und Vorrichtung zur Ausfuehrung des Verfahrens |
JPS4823385A (enrdf_load_stackoverflow) * | 1971-07-28 | 1973-03-26 | ||
DE2151167C3 (de) * | 1971-10-14 | 1974-05-09 | Siemens Ag, 1000 Berlin Und 8000 Muenchen | Elektronenstrahl-Mikroanalysator mit Auger-Elektronen-Nachweis |
US3796947A (en) * | 1973-02-27 | 1974-03-12 | Bell Telephone Labor Inc | Electron beam testing of film integrated circuits |
US4169244A (en) * | 1978-02-03 | 1979-09-25 | Plows Graham S | Electron probe testing, analysis and fault diagnosis in electronic circuits |
DE2814049A1 (de) * | 1978-03-31 | 1979-10-18 | Siemens Ag | Verfahren zur beruehrungslosen messung des potentialverlaufs in einem elektronischen bauelement und anordnung zur durchfuehrung des verfahrens |
DE2823642A1 (de) * | 1978-05-30 | 1980-01-03 | Siemens Ag | Verfahren zur beruehrungslosen potentialmessung an einem elektronischen bauelement |
US4179604A (en) * | 1978-09-29 | 1979-12-18 | The United States Of America As Represented By The Secretary Of The Navy | Electron collector for forming low-loss electron images |
JPS55156867A (en) * | 1979-05-28 | 1980-12-06 | Hitachi Ltd | Potential measuring device |
US4417203A (en) * | 1981-05-26 | 1983-11-22 | International Business Machines Corporation | System for contactless electrical property testing of multi-layer ceramics |
-
1981
- 1981-09-30 DE DE19813138929 patent/DE3138929A1/de not_active Withdrawn
-
1982
- 1982-07-15 US US06/398,542 patent/US4514682A/en not_active Expired - Fee Related
- 1982-08-17 EP EP82107490A patent/EP0075709B1/de not_active Expired
- 1982-08-17 DE DE8282107490T patent/DE3276035D1/de not_active Expired
- 1982-09-27 JP JP57168239A patent/JPS5871542A/ja active Granted
Non-Patent Citations (1)
Title |
---|
"Scanning Electron Microscopy", 1971/1, p.285-296 (SEM/nc, AMF O'Hare, USA) * |
Also Published As
Publication number | Publication date |
---|---|
DE3276035D1 (en) | 1987-05-14 |
US4514682A (en) | 1985-04-30 |
EP0075709A3 (en) | 1983-06-29 |
JPS5871542A (ja) | 1983-04-28 |
EP0075709A2 (de) | 1983-04-06 |
DE3138929A1 (de) | 1983-04-14 |
JPS6352428B2 (enrdf_load_stackoverflow) | 1988-10-19 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
DE4019005C2 (de) | Vorrichtungen zur Analyse von Ionen hoher Masse | |
EP0104577B1 (de) | Verfahren zur kontaktlosen Prüfung eines Objekts, insbesondere von Mikroverdrahtungen, mit einer Korpuskularstrahl-Sonde | |
EP0205184B1 (de) | Abberrationsarmes Spektrometer-Objektiv hoher Sekundärelektronen-Akzeptanz | |
EP0189777B1 (de) | Korpuskularstrahl-Messverfahren zum berührungslosen Testen von Leitungsnetzwerken | |
EP0075709B1 (de) | Spektrometer zum Nachweis der von einer Elektronensonde auf einer Probe ausgelösten Sekundärelektronen | |
EP0194570A2 (de) | Raster-Korpuskularmikroskop mit verringertem Boersch-Effekt | |
EP0013876B1 (de) | Einrichtung zur berührungslosen Potentialmessung | |
EP0274622A1 (de) | Detektoranordnung mit einem Detektorobjektiv für Korpuskularstrahlgeräte | |
EP0075716B1 (de) | Verbessertes Gegenfeld-Spektrometer für die Elektronenstrahl-Messtechnik | |
DE196958T1 (de) | Elektronenstrahlpruefsonde zur untersuchung integrierter schaltungen. | |
DE69607543T2 (de) | Detektoren für geladene Teilchen sowie diese verwendende Massenspektrometer | |
DE3532781A1 (de) | Anordnung zur detektion von sekundaer- und/oder rueckstreuelektronen in einem elektronenstrahlgeraet | |
DE69410133T2 (de) | Mehrdetektorsystem für die Detektion geladener Partikel | |
EP1801844A2 (de) | Verfahren und Vorrichtung zur Abstandsmessung | |
DE19635645C2 (de) | Verfahren für die hochauflösende Spektrenaufnahme von Analytionen in einem linearen Flugzeitmassenspektrometer | |
DE2011193C3 (de) | Vorrichtung für die Elektronen-Rastermikroskopie und die Elektronenstrahl-Mikroanalyse | |
EP0205185A2 (de) | Spektrometer-Objektiv für die Elektronenstrahl-Messtechnik | |
DE2706629C3 (de) | Einrichtung zur Überwachung der Position und der räumlichen Verteilung eines Elektronenstrahlbündels hoher Energie | |
EP0172477A2 (de) | Verfahren und Vorrichtung zur Registrierung von Teilchen oder Quanten mit Hilfe eines Detektors | |
EP0472938B1 (de) | Anordnung zum Testen und Reparieren einer integrierten Schaltung | |
DE69028647T2 (de) | Energieanalysator für geladene Teilchen | |
DE3873399T2 (de) | Oberflaechenanalysegeraet. | |
EP0232790A1 (de) | Verfahren und Anordnung zur Messung zeitabhängiger Signale mit einer Korpuskularsonde | |
DE3781963T2 (de) | Oberflaechenanalysegeraet. | |
DE2414221C3 (de) | Ionenoptisches Gerät zur Untersuchung der Oberfläche einer Probe durch IonenbeschuB und Analyse der vom beschossenen Oberflächenbereich ausgehenden Ionen |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
AK | Designated contracting states |
Designated state(s): DE FR GB NL |
|
PUAL | Search report despatched |
Free format text: ORIGINAL CODE: 0009013 |
|
AK | Designated contracting states |
Designated state(s): DE FR GB NL |
|
17P | Request for examination filed |
Effective date: 19831128 |
|
GRAA | (expected) grant |
Free format text: ORIGINAL CODE: 0009210 |
|
AK | Designated contracting states |
Kind code of ref document: B1 Designated state(s): DE FR GB NL |
|
REF | Corresponds to: |
Ref document number: 3276035 Country of ref document: DE Date of ref document: 19870514 |
|
ET | Fr: translation filed | ||
PGFP | Annual fee paid to national office [announced via postgrant information from national office to epo] |
Ref country code: NL Payment date: 19870831 Year of fee payment: 6 |
|
PLBE | No opposition filed within time limit |
Free format text: ORIGINAL CODE: 0009261 |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: NO OPPOSITION FILED WITHIN TIME LIMIT |
|
26N | No opposition filed | ||
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: GB Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES Effective date: 19880817 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: NL Effective date: 19890301 |
|
NLV4 | Nl: lapsed or anulled due to non-payment of the annual fee | ||
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: FR Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES Effective date: 19890428 |
|
PG25 | Lapsed in a contracting state [announced via postgrant information from national office to epo] |
Ref country code: DE Effective date: 19890503 |
|
GBPC | Gb: european patent ceased through non-payment of renewal fee | ||
REG | Reference to a national code |
Ref country code: FR Ref legal event code: ST |