EP0425052A1 - Photomultiplier tube comprising a stacked dynode multiplier and providing a high collection efficiency and reduced size - Google Patents
Photomultiplier tube comprising a stacked dynode multiplier and providing a high collection efficiency and reduced size Download PDFInfo
- Publication number
- EP0425052A1 EP0425052A1 EP90202838A EP90202838A EP0425052A1 EP 0425052 A1 EP0425052 A1 EP 0425052A1 EP 90202838 A EP90202838 A EP 90202838A EP 90202838 A EP90202838 A EP 90202838A EP 0425052 A1 EP0425052 A1 EP 0425052A1
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- EP
- European Patent Office
- Prior art keywords
- photocathode
- multiplier
- photomultiplier tube
- stackable
- dynodes
- 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.)
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J43/00—Secondary-emission tubes; Electron-multiplier tubes
- H01J43/04—Electron multipliers
- H01J43/06—Electrode arrangements
Definitions
- the present invention relates to a photomultiplier tube comprising a photocathode, an input electrode and an electron multiplier with stackable dynodes.
- the invention finds a particularly advantageous application in the field of photomultiplier tubes with electron multiplier with stackable dynodes.
- stacking multiplier dynode electron is meant all the multiplying devices having a layer structure as the multiplier of the type "sheet” (see e.g. French Patent No. 2549288) or the multipliers dynodes shutters in which each dynode consists of parallel blades inclined relative to the axis of the multiplier.
- a general technical problem which arises in any photomultiplier tube is to ensure the largest possible collection of photoelectrons from the photocathode.
- this general technical problem is coupled with another problem, namely that of coupling the first dynode to the multiplier device so that the secondary electrons emitted by the photocathode can arrive with little loss to the stacking dynode multiplier.
- the known photomultiplier tube of the state of the art has the disadvantage of a relatively large lateral size, mainly due to the fact that, given the fairly large dimensions of the first dynode and the dispersion of the secondary electrons emitted by the latter, the leaf multiplier cannot be placed in the immediate vicinity of the first dynode.
- this known tube also has the drawback of a large longitudinal bulk, linked to the need to have a sufficient distance between the photocathode and the first dynode, to allow the input electrode to focus d 'ensure its photoelectron concentration function on the first dynode.
- the technical problem to be solved by the object of the present invention is to provide a photomultiplier tube comprising a photocathode deposited on an entry window sealed at one end of a sleeve, an entry electrode, and a multiplier d electrons with stackable dynodes, tube through which a very high collection efficiency could be obtained, that is to say a perfect coupling between the photocathode and the electron multiplier with stackable dynodes, while offering lateral bulk and reduced longitudinal.
- the solution to the technical problem posed consists, according to the present invention, in that said input electrode comprises a truncated cone of conductor inside which is placed the electron multiplier with stackable dynodes.
- the electron multiplier with stackable dynodes occupying a central position in the tube, the lateral bulk is considerably reduced.
- the ideal coupling situation is achieved between the photocathode and the multiplier, and therefore d perfect collection efficiency, since, in the space between the photocathode and the input electrode-multiplier assembly, the accelerating electric field of the photoelectrons comes essentially from the first dynode of the stackable dynode multiplier. Insofar as the electrons produced by the photocathode inevitably reach the multiplier, it is possible to envisage bringing said multiplier closer to the photocathode, thereby reducing the longitudinal dimensions of the tube.
- the photomultiplier tube according to the invention is further characterized in that it comprises at least one generator of a material constituting the photocathode placed in the space located between the electrode inlet and sleeve.
- the generator of material constituting the photocathode is kept relatively distant from said photocathode by taking advantage of the space left free between the input electrode and the sleeve, due to the truncated cone shape given to said electrode d 'Entrance. This arrangement makes it possible to obtain very homogeneous photocathodes despite the reduction in length of the tube.
- FIG. 1 shows, in section, a photomultiplier tube comprising a photocathode 10, made of alkali antimonide for example, deposited on an inlet window 20 sealed at one end of a cylindrical sleeve 30.
- the photocathode 10 emits photoelectrons 11 which must reach, for secondary multiplication purposes, an electron multiplier 50, with stackable dynodes, whose multiplication axis is substantially coincident with l axis of the cylindrical sleeve 30.
- An example of an electron multiplier with stackable dynodes which could be suitable for the present invention is described in patent application FR-A-2 549 288.
- An anode 80 placed at the output of the multiplier 50 collects the electrons resulting from the multiplication by the stackable dynodes.
- the photomultiplier tube also includes an input electrode 40 constituted by a conductive truncated cone inside which is placed the electron multiplier 50.
- the photocathode is brought to the potential V1, which will be taken equal to 0V
- the first dynode 51 of the multiplier 50 is at a potential V3 of approximately 300 V
- the input electrode 40 has a potential V2 from 0 to 25 V, and generally less than 10% of the potential V3.
- the cathode 10 being brought to the potential V1
- the potential V2 of the input electrode 40 is between V1 and V1 increased by 10% of the difference between the potential V3 of the first dynode 51 of the multiplier 50 and the potential V1 of the photocathode 10.
- all the electrons 11 emitted by the photocathode 10 are captured by the first stackable dynode 51 since, in the space of input of the tube, the electric field is produced exclusively by said first dynode 51 at potential V3.
- the coupling and the collection are perfect, whatever the value of V3 and the distance between the photocathode 10 and the multiplier 50.
- the multiplier 50 can therefore bring the multiplier 50 closer to the photocathode 10 without harming the collection, resulting in a shorter tube.
- the section of the tube can be reduced because the coupling is independent of the incidence of electrons. Therefore, the useful input area can be limited to the small area in itself of the stackable dynodes.
- the theoretical limit to reducing the photocathode-multiplier distance of a photomultiplier tube is the possibility of producing, at least partially, the photocathode using generators of material constituting said photocathode. Indeed, these generators, antimony grains in particular, must be placed opposite the photocathode and relatively distant from the latter to obtain a homogeneous photocathode. As illustrated in FIG. 1, it is possible to satisfy this requirement while maintaining the electron multiplier 50 near photocathode 10 by placing said generators 61, 62 in the space 70 located between electrode 40 d entry and the sleeve 30. As shown by the arrows from the generator 61, the antimony produced by the generators 61 and 62 can cover the photocathode 10 homogeneously.
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- Common Detailed Techniques For Electron Tubes Or Discharge Tubes (AREA)
Abstract
Description
La présente invention concerne un tube photomultiplicateur comportant une photocathode, une électrode d'entrée et un multiplicateur d'électrons à dynodes empilables.The present invention relates to a photomultiplier tube comprising a photocathode, an input electrode and an electron multiplier with stackable dynodes.
L'invention trouve une application particulièrement avantageuse dans le domaine des tubes photomultiplicateurs à multiplicateur d'électrons à dynodes empilables. Par "multiplicateur d'électrons à dynodes empilables", on entend tous les dispositifs multiplicateurs à structure lamellaire comme les multiplicateurs du type "à feuilles" (voir par exemple le brevet français no 2 549 288) ou encore les multiplicateurs à dynodes en persiennes dans lesquels chaque dynode est constituée de lames parallèles inclinées par rapport à l'axe du multiplicateur.The invention finds a particularly advantageous application in the field of photomultiplier tubes with electron multiplier with stackable dynodes. By "stacking multiplier dynode electron" is meant all the multiplying devices having a layer structure as the multiplier of the type "sheet" (see e.g. French Patent No. 2549288) or the multipliers dynodes shutters in which each dynode consists of parallel blades inclined relative to the axis of the multiplier.
Un problème technique général qui se pose à tout tube photomultiplicateur est d'assurer une collection des photoélectrons issus de la photocathode qui soit la plus grande possible. Dans le cas des tubes comportant un dispositif multiplicateur à dynodes empilables, ce problème technique général se double d'un autre problème, à savoir celui de coupler la première dynode au dispositif multiplicateur de sorte que les électrons secondaires émis par la photocathode puissent parvenir avec peu de perte au dispositif multiplicateur à dynodes empilables.A general technical problem which arises in any photomultiplier tube is to ensure the largest possible collection of photoelectrons from the photocathode. In the case of tubes comprising a multiplier device with stackable dynodes, this general technical problem is coupled with another problem, namely that of coupling the first dynode to the multiplier device so that the secondary electrons emitted by the photocathode can arrive with little loss to the stacking dynode multiplier.
Une solution à ce double problème technique est donnée, par exemple, dans le brevet français no 2 549 288 (figure 12), qui décrit un tube photomultiplicateur conforme au préambule, et dont la première dynode est cylindrique, de génératrices orthogonales à l'axe du tube. Dans ce tube connu, le couplage entre la première dynode et le dispositif multiplicateur d'électrons à dynodes empilables du type "à feuilles" est réalisé en plaçant le multiplicateur en sortie de la première dynode, l'axe du multiplicateur à feuilles étant disposé perpendiculairement à l'axe du tube. Ainsi, dans cette configuration, le dispositif multiplicateur offre la plus grande section de capture aux électrons secondaires émis par la première dynode, d'où une bonne efficacité de collection.One solution to this double technical problem is given, for example, in French Patent No. 2,549,288 (Figure 12), which describes a photomultiplier tube according to the preamble, and the first dynode is cylindrical, with generatrices orthogonal to the axis of the tube. In this known tube, the coupling between the first dynode and the electron multiplier device with stackable dynodes of the "leaf" type is carried out by placing the multiplier at the outlet. of the first dynode, the axis of the leaf multiplier being arranged perpendicular to the axis of the tube. Thus, in this configuration, the multiplier device offers the largest capture section to the secondary electrons emitted by the first dynode, hence good collection efficiency.
Toutefois, le tube photomultiplicateur connu de l'état de la technique présente l'inconvénient d'un encombrement latéral relativement grand, dû principalement au fait que, compte-tenu des dimensions assez importantes de la première dynode et de la dispersion des électrons secondaires émis par cette dernière, le multiplicateur à feuilles ne peut être placé à proximité immédiate de la première dynode. De plus, il faut prévoir un dégagement vers l'arrière du multiplicateur pour les connexions de sortie, ce qui contribue à augmenter les dimensions du manchon servant d'enveloppe au tube.However, the known photomultiplier tube of the state of the art has the disadvantage of a relatively large lateral size, mainly due to the fact that, given the fairly large dimensions of the first dynode and the dispersion of the secondary electrons emitted by the latter, the leaf multiplier cannot be placed in the immediate vicinity of the first dynode. In addition, it is necessary to provide a rearward clearance of the multiplier for the outlet connections, which contributes to increasing the dimensions of the sleeve serving as an envelope for the tube.
Par ailleurs, ce tube connu présente également l'inconvénient d'un encombrement longitudinal important, lié à la nécessité de devoir disposer d'une distance suffisante entre la photocathode et la première dynode, pour permettre à l'électrode d'entrée de focalisation d'assurer sa fonction de concentration des photoélectrons sur la première dynode.Furthermore, this known tube also has the drawback of a large longitudinal bulk, linked to the need to have a sufficient distance between the photocathode and the first dynode, to allow the input electrode to focus d 'ensure its photoelectron concentration function on the first dynode.
Aussi, le problème technique à résoudre par l'objet de la présente invention est de proposer un tube photomultiplicateur comportant une photocathode déposée sur une fenêtre d'entrée scellée à une extrémité d'un manchon, une électrode d'entrée, et un multiplicateur d'électrons à dynodes empilables, tube grâce auquel on pourrait obtenir une efficacité de collection très élevée, c'est-à-dire un couplage parfait entre la photocathode et le multiplicateur d'électrons à dynodes empilables, tout en offrant un encombrement latéral et longitudinal réduit.Also, the technical problem to be solved by the object of the present invention is to provide a photomultiplier tube comprising a photocathode deposited on an entry window sealed at one end of a sleeve, an entry electrode, and a multiplier d electrons with stackable dynodes, tube through which a very high collection efficiency could be obtained, that is to say a perfect coupling between the photocathode and the electron multiplier with stackable dynodes, while offering lateral bulk and reduced longitudinal.
La solution au problème technique posé consiste, selon la présente invention en ce que ladite électrode d'entrée comporte un tronc de cône conducteur à l'intérieur duquel est disposé le multiplicateur d'électrons à dynodes empilables.The solution to the technical problem posed consists, according to the present invention, in that said input electrode comprises a truncated cone of conductor inside which is placed the electron multiplier with stackable dynodes.
Ainsi, d'une part, le multiplicateur d'électrons à dynodes empilables occupant une position centrale dans le tube, l'encombrement latéral se trouve sensiblement réduit. D'autre part, comme on le verra plus loin en détail, en appliquant à l'électrode d'entrée un potentiel électrique voisin de celui de la photocathode, on réalise la situation de couplage idéal entre la photocathode et le multiplicateur, et donc d'efficacité de collection parfaite, puisque, dans l'espace situé entre la photocathode et l'ensemble électrode d'entrée-multiplicateur, le champ électrique accélérateur des photoélectrons provient essentiellement de la première dynode du multiplicateur à dynodes empilables. Dans la mesure où les électrons produits par la photocathode parviennent immanquablement jusqu'au multiplicateur, on peut envisager de rapprocher ledit multiplicateur de la photocathode, d'où une réduction de l'encombrement longitudinal du tube.Thus, on the one hand, the electron multiplier with stackable dynodes occupying a central position in the tube, the lateral bulk is considerably reduced. On the other hand, as will be seen in detail below, by applying an electrical potential close to that of the photocathode to the input electrode, the ideal coupling situation is achieved between the photocathode and the multiplier, and therefore d perfect collection efficiency, since, in the space between the photocathode and the input electrode-multiplier assembly, the accelerating electric field of the photoelectrons comes essentially from the first dynode of the stackable dynode multiplier. Insofar as the electrons produced by the photocathode inevitably reach the multiplier, it is possible to envisage bringing said multiplier closer to the photocathode, thereby reducing the longitudinal dimensions of the tube.
Selon un mode préféré de mise en oeuvre, le tube photomultiplicateur selon l'invention est caractérisé en outre en ce qu'il comporte au moins un générateur d'un matériau constitutif de la photocathode placé dans l'espace situé entre l'électrode d'entrée et le manchon. Le générateur de matériau constitutif de la photocathode se trouve maintenu relativement éloigné de ladite photocathode en tirant parti de l'espace laissé libre entre l'électrode d'entrée et le manchon, du fait de la forme en tronc de cône donnée à ladite électrode d'entrée. Cette disposition permet l'obtention de photocathodes très homogènes malgré la réduction de longueur du tube.According to a preferred embodiment, the photomultiplier tube according to the invention is further characterized in that it comprises at least one generator of a material constituting the photocathode placed in the space located between the electrode inlet and sleeve. The generator of material constituting the photocathode is kept relatively distant from said photocathode by taking advantage of the space left free between the input electrode and the sleeve, due to the truncated cone shape given to said electrode d 'Entrance. This arrangement makes it possible to obtain very homogeneous photocathodes despite the reduction in length of the tube.
La description qui va suivre en regard du dessin annexé, donné à titre d'exemple non limitatif, fera bien comprendre en quoi consiste l'invention et comment elle peut être réalisée.
- La figure 1 est une vue en coupe d'un tube photomultiplicateur selon l'invention.
- Figure 1 is a sectional view of a photomultiplier tube according to the invention.
La figure 1 montre, en coupe, un tube photomultiplicateur comportant une photocathode 10, en antimoniure d'alcalins par exemple, déposée sur une fenêtre 20 d'entrée scellée à une extrémité d'un manchon 30 cylindrique. Sous l'effet d'un rayonnement lumineux incident, la photocathode 10 émet des photoélectrons 11 qui doivent atteindre, aux fins de multiplication secondaire, un multiplicateur 50 d'électrons, à dynodes empilables, dont l'axe de multiplication est sensiblement confondu avec l'axe du manchon 30 cylindrique. Un exemple de multiplicateur d'électrons à dynodes empilables qui pourrait convenir à la présente invention est décrit dans la demande de brevet FR-A-2 549 288. Une anode 80 placée en sortie du multiplicateur 50 recueille les électrons résultant de la multiplication par les dynodes empilables.FIG. 1 shows, in section, a photomultiplier tube comprising a photocathode 10, made of alkali antimonide for example, deposited on an
Comme l'indique la figure 1, le tube photomultiplicateur comporte également une électrode 40 d'entrée constituée par un tronc de cône conducteur à l'intérieur duquel est disposé le multiplicateur 50 d'électrons. En fonctionnement, la photocathode est portée au potentiel V₁, que l'on prendra égal à 0V, la première dynode 51 du multiplicateur 50 est à un potentiel V₃ de 300 V environ, tandis que l'électrode 40 d'entrée a un potentiel V₂ de 0 à 25 V, et d'une façon générale moins de 10% du potentiel V₃. De manière générale, selon l'invention la cathode 10 étant portée au potentiel V₁, le potentiel V₂ de l'électrode 40 d'entrée est compris entre V₁ et V₁ augmenté de 10% de la différence entre le potentiel V₃ de la première dynode 51 du multiplicateur 50 et le potentiel V₁ de la photocathode 10. Si l'électrode d'entrée est à V₂ = V₁, tous les électrons 11 émis par la photocathode 10 sont capturés par la première dynode empilable 51 puisque, dans l'espace d'entrée du tube, le champ électrique est produit exclusivement par ladite première dynode 51 au potentiel V₃. Le couplage et la collection sont parfaits, quelque soit la valeur de V₃ et la distance entre la photocathode 10 et le multiplicateur 50. On peut donc rapprocher le multiplicateur 50 de la photocathode 10 sans nuire à la collection, d'où un tube plus court. De même, la section du tube peut être réduite du fait que le couplage est indépendant de l'incidence des électrons. Par conséquent, la surface d'entrée utile peut être limitée à la surface, petite en elle-même, des dynodes empilables.As shown in FIG. 1, the photomultiplier tube also includes an input electrode 40 constituted by a conductive truncated cone inside which is placed the
On observe cependant qu'avec des potentiels V₁ et V₂ égaux, la réponse temporelle du tube n'est pas très bonne car le temps de transit des photoélectrons peut varier notablement entre les électrons issus du centre de la photocathode 11 et ceux provenant des bords. C'est pour remédier à cet inconvénient qu'on envisage également de porter l'électrode 40 d'entrée à un potentiel V₂ de 25 V par exemple, (V₁ étant supposé égal à 0 Volt) qui améliore le temps de réponse du tube sans dégrader sensiblement l'efficacité de collection.It is observed however that with equal potentials V₁ and V₂, the temporal response of the tube is not very good because the transit time of the photoelectrons can vary notably between the electrons coming from the center of
La limite théorique à la réduction de la distance photocathode-multiplicateur d'un tube photomultiplicateur est la possibilité de réaliser, au moins partiellement, la photocathode à l'aide de générateurs de matériau constitutif de ladite photocathode. En effet ces générateurs, grains d'antimoine notamment, doivent être placés en regard de la photocathode et relativement éloignés de celle-ci pour obtenir une photocathode homogène. Comme l'illustre la figure 1, il est possible de satisfaire à cette exigence tout en maintenant le multiplicateur 50 d'électrons à promixité de la photocathode 10 en plaçant lesdits générateurs 61, 62 dans l'espace 70 situé entre l'électrode 40 d'entrée et le manchon 30. Ainsi que le montre les flèches issues du générateur 61, l'antimoine produit par les générateurs 61 et 62 peut recouvrir la photocathode 10 de façon homogène.The theoretical limit to reducing the photocathode-multiplier distance of a photomultiplier tube is the possibility of producing, at least partially, the photocathode using generators of material constituting said photocathode. Indeed, these generators, antimony grains in particular, must be placed opposite the photocathode and relatively distant from the latter to obtain a homogeneous photocathode. As illustrated in FIG. 1, it is possible to satisfy this requirement while maintaining the
Claims (3)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
FR8914143 | 1989-10-27 | ||
FR8914143A FR2653934A1 (en) | 1989-10-27 | 1989-10-27 | PHOTOMULTIPLIER TUBE COMPRISING A MULTIPLIER WITH STACKABLE DYNODES AND HAVING HIGH COLLECTION EFFICIENCY AND REDUCED SIZE. |
Publications (1)
Publication Number | Publication Date |
---|---|
EP0425052A1 true EP0425052A1 (en) | 1991-05-02 |
Family
ID=9386869
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP90202838A Withdrawn EP0425052A1 (en) | 1989-10-27 | 1990-10-24 | Photomultiplier tube comprising a stacked dynode multiplier and providing a high collection efficiency and reduced size |
Country Status (4)
Country | Link |
---|---|
US (1) | US5126551A (en) |
EP (1) | EP0425052A1 (en) |
JP (1) | JPH03171543A (en) |
FR (1) | FR2653934A1 (en) |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2728014A (en) * | 1951-04-26 | 1955-12-20 | Rca Corp | Electron lens for multiplier phototubes with very low spherical aberration |
US2908840A (en) * | 1955-09-01 | 1959-10-13 | Rca Corp | Photo-emissive device |
DE1464882A1 (en) * | 1964-06-19 | 1969-10-16 | Akad Wissenschaften Ddr | Photomultiplier without pre-pulses, especially for short-term measurement and processes for its manufacture |
EP0264992A1 (en) * | 1986-10-03 | 1988-04-27 | Philips Composants | Segmented photomultiplier tube |
US4855642A (en) * | 1988-03-18 | 1989-08-08 | Burle Technologies, Inc. | Focusing electrode structure for photomultiplier tubes |
EP0345888A1 (en) * | 1988-06-10 | 1989-12-13 | Philips Photonique | Coupling device between the first dynode of a photomultiplier and a sheet multiplier |
Family Cites Families (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3668388A (en) * | 1971-02-24 | 1972-06-06 | Gte Sylvania Inc | Multi-channel photomultiplier tube |
US4333031A (en) * | 1979-03-30 | 1982-06-01 | Rca Corporation | Photomultiplier tube having directional alkali metal vapor evaporation means |
FI75948C (en) * | 1983-10-28 | 1988-08-08 | Wallac Oy | FOTOMULTIPLIKATOR FOER ANVAENDNING VID VAETSKESCINTILLATIONSRAEKNING. |
JP2516995B2 (en) * | 1987-08-05 | 1996-07-24 | 浜松ホトニクス株式会社 | Photomultiplier tube |
-
1989
- 1989-10-27 FR FR8914143A patent/FR2653934A1/en active Pending
-
1990
- 1990-10-23 US US07/603,972 patent/US5126551A/en not_active Expired - Fee Related
- 1990-10-24 JP JP2284503A patent/JPH03171543A/en active Pending
- 1990-10-24 EP EP90202838A patent/EP0425052A1/en not_active Withdrawn
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2728014A (en) * | 1951-04-26 | 1955-12-20 | Rca Corp | Electron lens for multiplier phototubes with very low spherical aberration |
US2908840A (en) * | 1955-09-01 | 1959-10-13 | Rca Corp | Photo-emissive device |
DE1464882A1 (en) * | 1964-06-19 | 1969-10-16 | Akad Wissenschaften Ddr | Photomultiplier without pre-pulses, especially for short-term measurement and processes for its manufacture |
EP0264992A1 (en) * | 1986-10-03 | 1988-04-27 | Philips Composants | Segmented photomultiplier tube |
US4855642A (en) * | 1988-03-18 | 1989-08-08 | Burle Technologies, Inc. | Focusing electrode structure for photomultiplier tubes |
EP0345888A1 (en) * | 1988-06-10 | 1989-12-13 | Philips Photonique | Coupling device between the first dynode of a photomultiplier and a sheet multiplier |
Also Published As
Publication number | Publication date |
---|---|
FR2653934A1 (en) | 1991-05-03 |
JPH03171543A (en) | 1991-07-25 |
US5126551A (en) | 1992-06-30 |
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