US3179835A - Pickup tube having a cesiated photocathode and a substantially leakagefree target, and method of making the same - Google Patents

Pickup tube having a cesiated photocathode and a substantially leakagefree target, and method of making the same Download PDF

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US3179835A
US3179835A US70988A US7098860A US3179835A US 3179835 A US3179835 A US 3179835A US 70988 A US70988 A US 70988A US 7098860 A US7098860 A US 7098860A US 3179835 A US3179835 A US 3179835A
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target
cesium
tube
antimony
manganese
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US70988A
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Paul W Kaseman
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RCA Corp
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RCA Corp
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J29/00Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
    • H01J29/02Electrodes; Screens; Mounting, supporting, spacing or insulating thereof
    • H01J29/10Screens on or from which an image or pattern is formed, picked up, converted or stored
    • H01J29/36Photoelectric screens; Charge-storage screens
    • H01J29/38Photoelectric screens; Charge-storage screens not using charge storage, e.g. photo-emissive screen, extended cathode

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  • This invention relates to a photosurface, and particularly to a photoemissive surface which may be especially useful for a photoemissive cathode and a method of making the same for use in a pickup or camera tube for television.
  • hit is a further object of this invention to provide a r l Target leakage is fixing the cesium by oxygen treatment.
  • FIG. 4 is a flow chart of a method of making the photosunface of the photocathode of FIG. 3.
  • the particular photosensitive surface which is the suborthicon type in which a transparent photoca-thode is used andthe supporting surface is that of the end of the tube.
  • FIG. 1 a television pickup tube 10 utilizing a photoemissive surface made in accordance with this invention.
  • a scene which is to be televised is focused upon the end plate 30 of the tube envelope l0.
  • Photoelectrons are released from a semi-trans arent photoemissive surface 31, formed on the inner sur iace of the face plate 30.
  • the photoelectrons are accelerated through an image section '12 by a ring electrode 32 so that they will strike a surface of a thin target 24, usually made of 24 and functions as a collector electrode electron emission.
  • the secondary electron emission from the sunfiace of the glass target 24 leaves a-positive charge pattern on the glass target su ace corresponding to the optical image focused upon the photocatbode 31.
  • the opposite side of the glass target 24, remote from photocathode 31, is scanned by an electron beam formed by an electron gun structure (not shown in detail), positioned in the otherend of the envelope 10 and including a final accelerating electrode 20.
  • the electron m is caused to approach the opposite side of target 24 at close to zero velocity through the use of a decelerating electrode 22. Due to the extreme thinness of the glass target 24, the electrostatic pattern on the photocathode side of the target 24 establishes the same image potential pattern on this opposite side of the target 24, he, the side toward the electron beam. Electrons from the cathode ray beam are the target surface and will be depositedon the positive areas of the target to neutralize for the secondary 30 either before or after the electrode is sealed into the envelope. in both cases is similar. It has been mount structure found, however,
  • t e manganese oxide appears to take up water yapor, if exposed to the atmosphere before the tube has been scaled.
  • a filament or pellet 42 (FIG. 1), of pure the positive The method of formation t manganese metal, is mounted within the cylindrical accelerating electrode 26 and beyond the peripheral edge of the mesh 34.
  • One end of the filament 42 is connected to the lead 46 and to a stem pin 48 (FIG. 2).
  • the other end of the manganese filament is connected to the inner surface of the accelerating electrode 26.
  • the filament 42 may be commercial grade electrolytic manganese, consisting of pure manganese having a maximum of approximately 0.1% of sulfur and iron.
  • the filament 42 is mounted close to the face plate 30 upon which the photosurface is to be formed when the manganese is evaporated from the filament 42.
  • Two or more filaments 42 may be arranged symmetrically about the axis of the supporting surface 30 for uniform distribution of the manganese.
  • the tube 10 in which the photosurface is to be formed is first processed and evacuated, and then baked between 375-400 C., for one hour to remove occluded gases from the envelope.
  • the metal electrodes within the tube are then heated and degassed, as is well known in the art. Also, the thermionic cathode is activated at this point.
  • a light source (not shown) is arranged above the tube end wall or face plate 30 and light directed through the envelope onto a photoelectric tube (not shown) to indicate the transparency of the face plate 30, and thus the amount of material deposited on the face plate may be indicated.
  • the indicator can be adjusted to show a scale reading of 100 at full transmission of the light through the envelope face plate 30. While the envelope is still being evacuated, a current is passed through the filament or pellet 42 by means of lead-in pins 48 and 52 to heat and evaporate the manganese therefrom. will condense upon the adjacent envelope wall portion and form a thin coating on the end wall 30.
  • the manganese metal is evaporated until the light transmission or transparency has been reduced to 90% of its original value.
  • This thickness of the manganese film is not critical and high sensitivity surfaces may be obtained with layers so thick as to afford 50% light transmission compared to the uncoated end wall or so thin as to afford 95% light transmission.
  • Oxygen is next introduced into the bulb through the exhaust tubulation, to a pressure of about 700 microns of mercury.
  • the transparent manganese film is oxidized by a high frequency wand (not shown) placed over the end wall 30.
  • the high frequency potential of the wand produces within the envelope a gaseous discharge which causes the manganese to react with the oxygen in the envelope.
  • the wand is moved over the end wall 30 for about two seconds. This method of oxidizing metal films within an envelope is well known and is fully described in Essig, US. Patent No. 2,020,305.
  • the oxygen in the envelope is then removed through the exhaust tubulation. At this time, the reading of the indicator that measured transmission through the face plate is then reset to indicate 100.
  • An antimony film is next put down over the oxidized manganese surface, also by evaporation of the antimony in vacuum.
  • An antimony containing filament (not shown) is also provided between one of the leads and the accelerating electrode 26 and within the electrode 26 similar to the manganese filament 42,
  • the antimony may be high grade commercial antimony having a composition of substantially 99.88% antimony and traces of iron, sulfur, arsenic and lead. Passing a current through the antimony filament evaporates the antimony and provides a film of antimony over the oxidized manganese deposit on the end wall 30. The evaporation of the antimony is continued until the light transmission through the end wall is approximately 50 to 85 percent of its value without the evaporated antimony layer.
  • Cesium is then released into the evacuated envelope by heating another container 54 having cesium therein and The evaporated manganesecathode and a target,
  • the released cesium permeates throughout the evacuated envelope and deposits over the antimony film on the end wall 30.
  • the cesium is evaporated to provide at least enough cesium to completely react with the total amount of antimony on the oxidized manganese on the end wall 30.
  • an excessive amount of cesium is preferably introduced into the envelope 10.
  • the tube is then baked in an oven, at a temperature of approximately between 120 C. and 200 C., to promote an activating reaction between the cesium and the antimony.
  • the tube is cooled to approximately room temperature. At this time sufiicient oxygen is introduced into the tube to fix any excess cesium. Although the phenomena is not exactly understood, it is believed that the excess cesium is fixed" by converting the free cesium into cesium-oxide.
  • An example of a means for fixing the free cesium in the tube is as follows: While the tube 10 is still on the exhaust system, oxygen is introduced into the tube until the pressure is approximately 15X 10- mm. of Hg. The oxygen is introduced in three doses, 2 or 3 seconds each, but not held so that the exhaust pump removes the oxygen shortly after its introduction.
  • This extra oxygen treatment fixes the cesium in the which are away from the photocathode without the photocathode itself.
  • the extra oxygen reacts with all of the free cesium within the envelope to form cesium oxide.
  • cesium oxide does not have the migrating properties of free cesium, the cesium oxide is fixed in its positions within the tube. Since the excess cesium is now fixed, target leakage in the image orthicon type pickup tube is eliminated while the photosurface still has its usual very high sensitivity.
  • the extra oxygen treatment has been found to make the tube more stable in that variations in photosurface sensitivity, with respect to time, are substantially eliminated.
  • the extra oxygen treatment has also been found to improve the blue sensitivity of the photosurface in tubes of this type.
  • a television pickup tube having a photosensitive said cathode comprising a transparent support base element, an oxidized manganese film on said base element, a deposit of antimony on said oxidized manganese film, and a deposit of cesium on sai deposit of antimony, said target comprising a relatively thin structure having thereon a deposit of cesium oxide, whereby said target is substantially free from leakage.
  • a method of making a pickup tube having an evacuated envelope enclosing a photoemissive cathode and a storage target the steps in the order recited of depositmg a layer of manganese velope, oxidizing said manganese, depositing antimony on said oxidized manganese, flashing at least enough cesium within said envelope to cesiate said antimony, whereby excess cesium is deposited on said target, and fixing said excess cesium on said target by exposing said excess cesium to oxygen, while substantially preserving said cathode from said oxygen.
  • a photosurface of the type including a manganese oxide layer having a cesiated-antimony layer thereon, and a layer of free cesium on said target depositing a photosurface of the type including a manganese oxide layer having a cesiated-antimony layer thereon, and a layer of free cesium on said target, and subsequently admitting oxygen into said tube to fix said free layer of cesium while substantially preserving said photosurface from said oxygen.
  • a method of making a camera tube of the type having a photosurface and a storage target the steps in the order recited of depositing manganese on a substrate, oxidizmg said manganese, depositing antimony on said oxidized manganese, cesiating said antimony in such a way on the face plate of said enand introducing oxygen into said tube for fixing substantially only said excess cesium on said target, whereby said target is substantially free from charge leakage thereacross.

Description

April 20, 1965 P. w, KASEMAN 3,179,835 PICKUP TUBE HAVING A CESIATED PHOTOCATHODE AND A SUBSTANTIALLY LEAKAGE-FREE TARGET, AND METHOD OF MAKING THE SAME Filed Nov. 22, 1960 Y 01/0/7770 0/ Ali/$6 465.92
&
mmvron. P10! W. f17J'iM4/V BY PICKUP TUBE HAVING A CESIATED PHOTO- CATHODE AND A SUBSTANTIALLY LEAKAGE- FREEAMETARGET, AND METHOD or MAKING THE Paul W. Kaseman, Lancaster, Pa., asslgnor to Radio Corporation of America, a corporation of Filed Nov. 22, 1960 S 4 Claims. oi.
This invention relates to a photosurface, and particularly to a photoemissive surface which may be especially useful for a photoemissive cathode and a method of making the same for use in a pickup or camera tube for television.
US. Patent No. this photosurface, which is a semi-transparent surface, is excellent for many Also, when processed in the last mentioned order, the photocathode of an stability due to pickup tube photosensitive sunface. The poor stability refers to the decrease in sensitivity of the target with respect to time.
It is therefore an object of this invention to provide an improved photosurfa It is another object of this invention to provide a photosensitive camera tube having a novel photocathode of improved sensitivity.
hit is a further object of this invention to provide a r l Target leakage is fixing the cesium by oxygen treatment.
will be more clearly understood by refaccompanying single sheet of drawings of the photoeathode of the and,.
3,179,335" Patented Apr. 20, 1965 2 tube shown in FIGS. 1 and 2; FIG. 4 is a flow chart of a method of making the photosunface of the photocathode of FIG. 3.
The particular photosensitive surface which is the suborthicon type in which a transparent photoca-thode is used andthe supporting surface is that of the end of the tube.
In FIG. 1 is shown a television pickup tube 10 utilizing a photoemissive surface made in accordance with this invention. In operation of the tube shown in FIG. 1, a scene which is to be televised is focused upon the end plate 30 of the tube envelope l0. Photoelectrons are released from a semi-trans arent photoemissive surface 31, formed on the inner sur iace of the face plate 30. The photoelectrons are accelerated through an image section '12 by a ring electrode 32 so that they will strike a surface of a thin target 24, usually made of 24 and functions as a collector electrode electron emission. The secondary electron emission from the sunfiace of the glass target 24 leaves a-positive charge pattern on the glass target su ace corresponding to the optical image focused upon the photocatbode 31. The opposite side of the glass target 24, remote from photocathode 31, is scanned by an electron beam formed by an electron gun structure (not shown in detail), positioned in the otherend of the envelope 10 and including a final accelerating electrode 20. The electron m is caused to approach the opposite side of target 24 at close to zero velocity through the use of a decelerating electrode 22. Due to the extreme thinness of the glass target 24, the electrostatic pattern on the photocathode side of the target 24 establishes the same image potential pattern on this opposite side of the target 24, he, the side toward the electron beam. Electrons from the cathode ray beam are the target surface and will be depositedon the positive areas of the target to neutralize for the secondary 30 either before or after the electrode is sealed into the envelope. in both cases is similar. It has been mount structure found, however,
t e manganese oxide appears to take up water yapor, if exposed to the atmosphere before the tube has been scaled. Before sealing the electrode mount structure into the envelope 10, a filament or pellet 42 (FIG. 1), of pure the positive The method of formation t manganese metal, is mounted within the cylindrical accelerating electrode 26 and beyond the peripheral edge of the mesh 34. One end of the filament 42 is connected to the lead 46 and to a stem pin 48 (FIG. 2). The other end of the manganese filament is connected to the inner surface of the accelerating electrode 26. The filament 42 may be commercial grade electrolytic manganese, consisting of pure manganese having a maximum of approximately 0.1% of sulfur and iron. In this manner, the filament 42 is mounted close to the face plate 30 upon which the photosurface is to be formed when the manganese is evaporated from the filament 42.. Two or more filaments 42 may be arranged symmetrically about the axis of the supporting surface 30 for uniform distribution of the manganese.
The tube 10, in which the photosurface is to be formed, is first processed and evacuated, and then baked between 375-400 C., for one hour to remove occluded gases from the envelope. The metal electrodes within the tube are then heated and degassed, as is well known in the art. Also, the thermionic cathode is activated at this point.
In order to measure the amount of material deposited on the inner surface of the face plate 30, a light source (not shown) is arranged above the tube end wall or face plate 30 and light directed through the envelope onto a photoelectric tube (not shown) to indicate the transparency of the face plate 30, and thus the amount of material deposited on the face plate may be indicated. The indicator can be adjusted to show a scale reading of 100 at full transmission of the light through the envelope face plate 30. While the envelope is still being evacuated, a current is passed through the filament or pellet 42 by means of lead-in pins 48 and 52 to heat and evaporate the manganese therefrom. will condense upon the adjacent envelope wall portion and form a thin coating on the end wall 30. The manganese metal is evaporated until the light transmission or transparency has been reduced to 90% of its original value. This thickness of the manganese film is not critical and high sensitivity surfaces may be obtained with layers so thick as to afford 50% light transmission compared to the uncoated end wall or so thin as to afford 95% light transmission.
Oxygen is next introduced into the bulb through the exhaust tubulation, to a pressure of about 700 microns of mercury. The transparent manganese film is oxidized by a high frequency wand (not shown) placed over the end wall 30. The high frequency potential of the wand produces within the envelope a gaseous discharge which causes the manganese to react with the oxygen in the envelope. The wand is moved over the end wall 30 for about two seconds. This method of oxidizing metal films within an envelope is well known and is fully described in Essig, US. Patent No. 2,020,305. The oxygen in the envelope is then removed through the exhaust tubulation. At this time, the reading of the indicator that measured transmission through the face plate is then reset to indicate 100.
An antimony film is next put down over the oxidized manganese surface, also by evaporation of the antimony in vacuum. An antimony containing filament (not shown) is also provided between one of the leads and the accelerating electrode 26 and within the electrode 26 similar to the manganese filament 42, The antimony may be high grade commercial antimony having a composition of substantially 99.88% antimony and traces of iron, sulfur, arsenic and lead. Passing a current through the antimony filament evaporates the antimony and provides a film of antimony over the oxidized manganese deposit on the end wall 30. The evaporation of the antimony is continued until the light transmission through the end wall is approximately 50 to 85 percent of its value without the evaporated antimony layer.
Cesium is then released into the evacuated envelope by heating another container 54 having cesium therein and The evaporated manganesecathode and a target,
mounted on a lead-in pin 60. The released cesium permeates throughout the evacuated envelope and deposits over the antimony film on the end wall 30. The cesium is evaporated to provide at least enough cesium to completely react with the total amount of antimony on the oxidized manganese on the end wall 30. In order to insure that all of the antimony has been cesiated, as a practical matter, an excessive amount of cesium is preferably introduced into the envelope 10. The tube is then baked in an oven, at a temperature of approximately between 120 C. and 200 C., to promote an activating reaction between the cesium and the antimony.
After the above steps have been performed, and while the tube is still on the exhaust system, the tube is cooled to approximately room temperature. At this time sufiicient oxygen is introduced into the tube to fix any excess cesium. Although the phenomena is not exactly understood, it is believed that the excess cesium is fixed" by converting the free cesium into cesium-oxide. An example of a means for fixing the free cesium in the tube is as follows: While the tube 10 is still on the exhaust system, oxygen is introduced into the tube until the pressure is approximately 15X 10- mm. of Hg. The oxygen is introduced in three doses, 2 or 3 seconds each, but not held so that the exhaust pump removes the oxygen shortly after its introduction.
This extra oxygen treatment fixes the cesium in the which are away from the photocathode without the photocathode itself. Thus, the extra oxygen reacts with all of the free cesium within the envelope to form cesium oxide. Since cesium oxide does not have the migrating properties of free cesium, the cesium oxide is fixed in its positions within the tube. Since the excess cesium is now fixed, target leakage in the image orthicon type pickup tube is eliminated while the photosurface still has its usual very high sensitivity. Also, the extra oxygen treatment has been found to make the tube more stable in that variations in photosurface sensitivity, with respect to time, are substantially eliminated. The extra oxygen treatment has also been found to improve the blue sensitivity of the photosurface in tubes of this type.
What is claimed is:
1. A television pickup tube having a photosensitive said cathode comprising a transparent support base element, an oxidized manganese film on said base element, a deposit of antimony on said oxidized manganese film, and a deposit of cesium on sai deposit of antimony, said target comprising a relatively thin structure having thereon a deposit of cesium oxide, whereby said target is substantially free from leakage.
2. In a method of making a pickup tube having an evacuated envelope enclosing a photoemissive cathode and a storage target, the steps in the order recited of depositmg a layer of manganese velope, oxidizing said manganese, depositing antimony on said oxidized manganese, flashing at least enough cesium within said envelope to cesiate said antimony, whereby excess cesium is deposited on said target, and fixing said excess cesium on said target by exposing said excess cesium to oxygen, while substantially preserving said cathode from said oxygen.
3. In a method of making a camera tube having a photosurface and a storage target, the steps of depositing a photosurface of the type including a manganese oxide layer having a cesiated-antimony layer thereon, and a layer of free cesium on said target, and subsequently admitting oxygen into said tube to fix said free layer of cesium while substantially preserving said photosurface from said oxygen. 1
4. In a method of making a camera tube of the type having a photosurface and a storage target, the steps in the order recited of depositing manganese on a substrate, oxidizmg said manganese, depositing antimony on said oxidized manganese, cesiating said antimony in such a way on the face plate of said enand introducing oxygen into said tube for fixing substantially only said excess cesium on said target, whereby said target is substantially free from charge leakage thereacross.
References Cited by the Exlmlner UNITED STATES PATENTS 1,935,894 11/33 Smith 313-l76 6 Kliever et a1 313102 Polkosky 313-102. Franks et al 313-102 X Dobischek et a1. 313-103 X Sommer 313-65 JAMES 1). KALLAM, Acting Primal) E'xmnlner. ARTHUR GAUSS, Examiner.

Claims (1)

1. A TELEVISION PICKUP TUBE HAVING A PHOTOSENSITIVE CATHODE AND A TARGET, SAID CATHODE COMPRISING A TRANSPARENT SUPPORT BASE ELEMENT, AN OXIDIZED MANGANESE FILM ON SAID BASE ELEMENT, A DEPOSIT OF ANTIMONY ON SAID OXIDIZED MANGANESE FILM, AND A DEPOSIT OF CESIUM ON SAID DEPOSIT OF ANTIMONY, SAID TARGET COMPRISING A RELATIVELY THIN STRUCTURE HAVING THEREON A DEPOSIT OF CESIUM OXIDE, WHEREBY SAID TARGET IS SUBSTANTIALLY FREE FROM LEAKAGE.
US70988A 1960-11-22 1960-11-22 Pickup tube having a cesiated photocathode and a substantially leakagefree target, and method of making the same Expired - Lifetime US3179835A (en)

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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3434876A (en) * 1965-11-23 1969-03-25 Rca Corp Photosensitive cathodes
US3658400A (en) * 1970-03-02 1972-04-25 Rca Corp Method of making a multialkali photocathode with improved sensitivity to infrared light and a photocathode made thereby

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1935894A (en) * 1929-03-25 1933-11-21 Raytheon Mfg Co Gaseous discharge device
US2601208A (en) * 1947-10-16 1952-06-17 Honeywell Regulator Co Photoelectric discharge device
US2676282A (en) * 1951-04-09 1954-04-20 Rca Corp Photocathode for multiplier tubes
US2754428A (en) * 1951-09-17 1956-07-10 George W Franks Electron discharge device
US2842706A (en) * 1956-03-01 1958-07-08 Dobischek Dietrich Cold cathode vacuum tube
US2914690A (en) * 1955-12-05 1959-11-24 Rca Corp Electron-emitting surfaces and methods of making them

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1935894A (en) * 1929-03-25 1933-11-21 Raytheon Mfg Co Gaseous discharge device
US2601208A (en) * 1947-10-16 1952-06-17 Honeywell Regulator Co Photoelectric discharge device
US2676282A (en) * 1951-04-09 1954-04-20 Rca Corp Photocathode for multiplier tubes
US2754428A (en) * 1951-09-17 1956-07-10 George W Franks Electron discharge device
US2914690A (en) * 1955-12-05 1959-11-24 Rca Corp Electron-emitting surfaces and methods of making them
US2842706A (en) * 1956-03-01 1958-07-08 Dobischek Dietrich Cold cathode vacuum tube

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3434876A (en) * 1965-11-23 1969-03-25 Rca Corp Photosensitive cathodes
US3658400A (en) * 1970-03-02 1972-04-25 Rca Corp Method of making a multialkali photocathode with improved sensitivity to infrared light and a photocathode made thereby

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