US3658400A

US3658400A - Method of making a multialkali photocathode with improved sensitivity to infrared light and a photocathode made thereby

Info

Publication number: US3658400A
Application number: US15742A
Authority: US
Inventors: Fred Anderson Helvy
Original assignee: RCA Corp
Current assignee: RCA Corp
Priority date: 1970-03-02
Filing date: 1970-03-02
Publication date: 1972-04-25
Anticipated expiration: 1989-04-25
Also published as: NL174098C; DE2109903C2; GB1345778A; NL174098B; FR2083948A5; CA930256A; NL7102696A; JPS5032194B1; DE2109903A1

Abstract

A method for making a multialkali photocathode includes simultaneous evaporation of sodium and antimony alternately with simultaneous evaporation of potassium and antimony. The disclosure includes a photocathode made by the method described.

Description

United Filed:

Mai. z, 1970 Appl. No.: 15,742

U.S. Cl.. 313/94, l17/33.5 CP, 316/5` 1l7/33.5 C, 33.5 CP, 219, 217; 313/65 R, 94

ates Patent 1151 3,658,400 Helvy 1451 Apr. 25, 1972 [54] METHOD 0F MAKING A [56] References Cited MULTIALKALI PHOTOCATHODE v UNITED STATES PATENTS WITH IMPROVE SENSITIVITY T0 2 431 401 11/1947 Janes ..316/6 x `INFRARED LIGHT ANDA 2,770,561 11/1956 sommer ...313/102 x PHOTOCATHODE MADE THEREBY 2,914,690 11/1959 sommer ...117/217 x 021 FfedAndefsonHelvy-Pa- 31133132? 311323 liiiii [73] Assignee: RCA Cdl-poration 3,498,834 3/1970 Rome et al ..1'17/217 Primary Examiner-John F. Campbell Assistant Examiner-Richard Bernard Lazarus Attorney-Glenn H. Bruestle described.

' lABSTRACT A method for making a muliialkali photocathode includes simultaneous evaporation of sodium and antmony alternately with simultaneous evaporation of potassium and antimony. The disclosure includes a photocathode made by the method 8 Claims, 3 Drawing Figures PATNTEDAPRZS 1912 Y 3,658,400 SHEET 10F 2 7447' MAX/MIM,- 7*//5/14 INVENTOR IBI/m19. MJ

#fiar/My METHOD OF MAKING A MULTIALKALI PIIOTOCATIIODE WITH IMPROVED SENSITIVITY TO INFRARED LIGHT AND A PI-IOTOCATIIODE MADE THEREBY BACKGROUND oF THE INVENTION require considerable skill on the part of the operator. Thus,

reproducibility may be poor, with the result that there may be a vsubstantial variance in theV response characteristics of finished surfaces. Moreover, photocathodes made by previous methods have little'sensitivity in the infrared region of the spectrum where wavelengths are 700 nanometers and longer. Yet, sensitivity to red and Vinfrared may be very desirable since, for example, many lasers commonly used for communications emit red or infrared light.

BRIEF DESCRIPTION oE'THE DRAWINGS of a preferred embodiment of the DESCRIPTION OF THE PREFERRED EMBODIMENTS General Tube Structure and Processing Equipment- FIG. l is a flow chart of steps 1-18 used for practicing a preferred embodiment of the novel method. By the steps l-l8, a phototube 26, shown in FIG. 2, is provided with a photocathode surface 28 having improved sensitivity to infrared light. The tube 26 has a tubular glass wall section 30 about inches long, 2 inches outside diameter and one-sixteenth inch thickness. One end of the wall section 30 is closed by a glass faceplate 32, which is flat on the outside and concave on the inside with a radius of curvature of about l.9 inches. The other end ofthe wall section 30 is closed by a stem 34 having a number of electrical lead-in pins 35. Along the interior of the tube are spaced a series of dynodes 36. Near the dynodes 36 are spaced three

channels

38,40, 42 of tantalum foil containing, respectively, substances for evaporating potassium, sodium, and cesium. The potassium channel 38 contains potassium chromate, aluminum, and tungsten. The sodium channel 40 contains sodium chromate, aluminum, and tungsten. The cesium channel 42 contains cesium chromate, zirconium and tungsten. A resistance filament situated near the faceplate has two antimony alloy beads 44 attached to it for evaporating antimony.l The

channels

38, 40, 42 and the filament 44 are suitably connected by internal leads to electrical current sources through the pins 35 so that they can be activated separately by electrical resistance heating.

Light transmission through the faceplate 32 is monitored by directing light from an incandescent tungsten filament at an angle through the faceplate 32 and Wall 30 to a light sensing tube. Photoemissive sensitivity of the interior faceplate surface is monitored by collecting the emitted electrons with one or more of the internal electrodes, such as the electrode 46. For such collection, the electrode 46 is impressed with a voltage of between 50 and 150 volts positive with respect to the photocathode 28 through a lead 48 going from a lead-in pin 35 to ari aluminum coating on the wall 30 and in contact with the photocathode 28 and lead 50 also from a lead-in pin 35 to the electrode 46. The sensitivity is expressed in terms of microamperes of emitted electron current per lumen of light incident on the photocathode 28.

During processing, the tube is continuously evacuated through exhausted tubulation 47 in the stem. The tubulation is of about l inch inside diameter and about 2 inches long. It

leads directly to a titanium evaporation-ion vacuum pump having a pumping speed of about 250 liters per second.

Processing Steps 3. The tube 26 is placed in an-oven which has been preheated to about 190 C.

4. While the tube 20 is heating to oven temperature, the

channels

38, 40, 42 are preheated to clean and degas them. Then the potassium channel 38 current is set so that the channel will release potassium vapor when the faceplate 32 temperature reaches about 180 C.

5. Potassium is evaporated on the antimony layer until maximum sensitivity is reached. The maximum is generally about l.5 l-5) microamperes per lumen.

6. The oven temperature is increased to about 220 (215- 230) C and the sodium channel 40 current adjusted so that sodium vapor willbe released when the faceplate 32 reaches about 210 (205220) C.

7. Sodium is evaporated until a maximum sensitivity is reached. The maximum is generally about 20 (l5-80) microamperes per lumen.

8. Sodium evaporation is continued and antimony is simultaneously evaporated until a maximum sensitivity is passed lat about 50 (4S-120) microamperes yper lumen and sensitivity has decreased to about l0 percent (5-15 percent) of the maximum. Then both evaporations are discontinued.

9. Potassium is evaporated until a maximum sensitivity is reached.

l0. Potassium evaporation is continued and antimony is simultaneously evaporated until the sensitivity decreases -to about l0 percent (5-l5 percent) of the maximum sensitivity in step 9.

ll. Steps 7 through 10 are repeated at least several times until the maximum sensitivity in step l0 is about 30 percent (2S-35 percent) of the highest maximum sensitivity reached in any of the previous steps 5 through 10. The photocathode will take on a light blue hue when the proper sensitivity for this step is reached.

l2. The tube 26 is cooled gradually to about 160 (155 -l65) C over a period of about 5 (5-10) minutes.

13. When the temperature reaches about 160 C, cesium is evaporated until the sensitivity passes a maximum and decreases to about percent (70-90 percent) of the maximum.

I4. The tube 26 is baked at 160 (l55-l65) C until a new maximum sensitivity is reached.

l5. Antimony is evaporated until the sensitivity decreases to about IO percent (5-15 percent) of the maximum reached in step 14).

I6. The tube is baked at (l55-l65) C until a new maximum sensitivity is reached.

I7. Steps 15) and 16) are repeated until the maximum sensitivity of step 16) stabilizes and the infrared sensitivity is between 0.5 and I6 microamperes per lumen.

I8. With the photocathode 28 completed, the tube 26 is slowly cooled to room temperature at a rate of about l0 C per minute and removed from the oven. After the exhaust tubulation 47 is sealed 0H, the tube 26 is operative.

GENERAL CONSIDERATIONS Techniques for monitoring sensitivity and light transmission during processing as well as for evaporating photocathode materials are further described, for instance in the U.S. Patents to A. H. Sommer and F. R. Hughes, referenced above, and also in U.S. Pat. No. 2,914,690 to A. H. Sommer and No. 2,676,282, to J. J. Polkosky.

Light transmission of the faceplate, for the purpose of monitoring the thickness of the antimony layer, is measured by conventional means. lts measurement is not critical.

Sensitivity of the evaporated layers is measured separately for visible light and infrared light. lt is desirable to be able to measure both visible and infrared sensitivity almost simultaneously so that the photocathode may be processed to give a favorable relative value of both sensitivities. For this purpose, two separate incandescent tungsten light sources are used, each about 0.1 lumen in output. The sources are spaced apart a short distance from the faceplate. Interposed between one source and the faceplate is a glass light filter passing infrared light but no visible light. For instance, a filter passing less than 0.025 percent at 750 nanometers wavelength, percent at 900 nanometers and about 90 percent at about 1,250 nanometers is suitable. The sensitivity of the photocathode to both visible and infrared light may be measured separately and almost simultaneously by manual switching from one light source to the other.

The rates of evaporation of the evaporated elements are limited by the speed and accuracy at which the sensitivity can be monitored. A relatively slow evaporation rate makes the monitoring less critical.

Maximum sensitivity is determined from the first derivative of the increasing sensitivity function. The first derivative takes a zero value at the peak of a sensitivity curve. A computer can be used to continually calculate the derivative of the sensitivity function, or a human operator can simply observe a plotted curve of the sensitivity and note when its tangent is horizontal to indicate a peak. However, in the course of an alkali metal evaporation there are often a number of spurious peaks in the sensitivity which are of lower values than a later highest maximum peak. In order to discriminate these spurious peaks from the maximum it is necessary to continue evaporation until the sensitivity has fallen to a value of about 80 percent of the sensitivity at the peak in question. It may then be assumed that the peak was the highest attainable for that evaporation and is therefore a maximum. A reference herein to evaporation of an alkali metal to a substantially maximum sensitivity means an evaporation past the maximum to at least l5 percent of the sensitivity at the maximum. Excess alkali metal evaporated after a maximum is reached generally evaporates off again during subsequent baking.

While in the preferred embodiment evaporation was done by heated channels inside the tube, external processing, such as is described in the aforementioned patents, can also be used to practice the novel method. Thus, the novel method can be used to form photocathodes having improved red response in tubes, such as image tubes for which internal processing may not be as useful as external processing because of possible contamination of electrodes.

The novel method results in high reproducibility of photocathodes and is thus particularly well suited for automated fabrication of photocathodes. With present methods, complete automation is not feasible because of a relatively low degree of reproducibility in the absence of a highly skilled operator. Furthermore, by the novel method it takes considerably less time, as much as 50 percent less, to make a multialkali photocathode than by present methods.

Present multialkali photocathodes have a thickness on the order of 30 nanometers, whereas photocathodes made by the novel method may have a thickness on the order of |50 nanometers. The greater thickness accounts in part for an increase in the sensitivity of the photocathode to red light, as shown in FIG. 3. The curve 52 in FIG. 3 represents the approximate response characteristic of a commonly used multialkali photocathode made by present methods. The response is seen to be quite low in the 700 nanometer wavelength region. The curve 54 represents the approximate response characteristic of a photocathode made by the novel method. lt is seen that the sensitivity is considerably higher in the 700 nanometer region and extends well beyond that region to as far as 950 nanometers 'in the infrared region. The high sensitivity in the infrared region is believed to be due to factors other than the photocathode thickness. In addition to the improved infrared response, the photocathode made by the novel method has a more nearly constant and higher sensitivity throughout the visual spectrum than present multialkali photocathodes.

Although the novel photocathode is made by a series of evaporations, it is presently not possible to define precisely the actual finished structure, since there is an alloying of the evaporated substances. The chemical compositions of the various thickness portions of the photocathode are not known. Therefore, the novel photocathode can presently be best described as the product of the novel method.

The novel photocathode may be used as a photoemitter on an opaque substrate or as a secondary electron emitting surface.

I claim:

l. Method of making a photocathode, comprising, in order:

a. forming a base layer containing antimony and potassium on a substrate;

b. evaporating sodium on said base layer until a sensitivity between 20 and 80 micro-amperes per lumen is attained',

c. continuing said evaporating of sodium while simultaneously evaporating antimony until the sensitivity passes a maximum and decreases to between 5 and 15 percent of the value at that maximum;

d. evaporating potassium until a substantially maximum sensitivity is attained;

e. continuing said evaporating of potassium while simultaneously evaporating antimony until the sensitivity passes a maximum and decreases to between 5 and l5 percent of that maximum; repeating, in order, the above steps b through e until the sensitivity is between 25 and 35 percent of the highest sensitivity previously reached in any of the steps b through e, and then g. sensitizing said photocathode by evaporating cesium,

baking, and then alternately evaporating antimony and baking until maximum sensitivities attained during said bakings after evaporating of said antimony are stabilized.

2. The method defined in claim 1 and wherein said step a of forming said base layer includes:

i. cleaning and degassing a transparent substrate surface by heating said substrate for at least 3 hours to a temperature of about 400 C in a vacuum;

ii. evaporating an antimony layer on said surface to a thickness which decreases the transmission of yellow visible light through said substrate by at least 5 percent;

iii. heating said surface to at least C;

iv. evaporating a potassium layer on said antimony layer until photoemission from said potassium layer is substantially maximum value.

3. The method defined in claim 1 and wherein said substrate is maintained at a temperature of between 200 and 250 C during said steps b through f.

4. The method defined in claim l and wherein said sensitizing includes:

h. cooling said substrate from the temperature at which said evaporating of potassium is carried out to a temperature sitivity of step 1 stabilizes to a value of at least 0.1 microampere per lumen for infrared light. 5. An electron emissive photocathode made by the method defined in claim l.

6. An electron emissive photocathode made by the method defined in claim 2.

7. An electron emissive photocathode made by the method defined in claim 3.

8. An electron emissive photocathode made by the method defined in claim 4.

Claims

2. The method defined in claim 1 and wherein said step a of forming said base layer includes: i. cleaning and degassing a transparent substrate suRface by heating said substrate for at least 3 hours to a temperature of about 400* C in a vacuum; ii. evaporating an antimony layer on said surface to a thickness which decreases the transmission of yellow visible light through said substrate by at least 5 percent; iii. heating said surface to at least 150* C; iv. evaporating a potassium layer on said antimony layer until photoemission from said potassium layer is substantially maximum value.
3. The method defined in claim 1 and wherein said substrate is maintained at a temperature of between 200* and 250* C during said steps b through f.
4. The method defined in claim 1 and wherein said sensitizing includes: h. cooling said substrate from the temperature at which said evaporating of potassium is carried out to a temperature of between 155* and 165* C over a period of between 5 and 10 minutes; i. evaporating cesium during said cooling until the sensitivity passes a maximum and decreases to between 70 and 90 percent of said maximum; j. baking said substrate until a new approximately maximum sensitivity is attained; k. evaporating antimony until the sensitivity decreases to 5 to 60 percent of said maximum sensitivity in step i; l. baking said substrate until a new approximately maximum sensitivity is attained; m. repeating steps k and l in order until said maximum sensitivity of step 1 stabilizes to a value of at least 0.1 micro-ampere per lumen for infrared light.
5. An electron emissive photocathode made by the method defined in claim 1.
6. An electron emissive photocathode made by the method defined in claim 2.
7. An electron emissive photocathode made by the method defined in claim 3.
8. An electron emissive photocathode made by the method defined in claim 4.