U.S. patent number 3,644,777 [Application Number 05/042,631] was granted by the patent office on 1972-02-22 for cathode-ray tube with serpentine-shaped transmission line deflection means.
Invention is credited to Vincent J. George, James B. Thomas.
United States Patent |
3,644,777 |
Thomas , et al. |
February 22, 1972 |
**Please see images for:
( Certificate of Correction ) ** |
CATHODE-RAY TUBE WITH SERPENTINE-SHAPED TRANSMISSION LINE
DEFLECTION MEANS
Abstract
Improved high-frequency response, cathode-ray tube for tracking,
determining, and recording high frequency, unknown input signals.
To this end, the invention provides a sectionalized, round and
square cross section CRT having ceramic, vacuumtight lead-ins;
impedance matched, insulated, serpentine traveling wave deflection
structures; and an electron gun incorporating an anode aperture
formed with a protrusion for providing high-electron beam
density.
Inventors: |
Thomas; James B. (Needham,
MA), George; Vincent J. (Winchester, MA) |
Assignee: |
|
Family
ID: |
21922942 |
Appl.
No.: |
05/042,631 |
Filed: |
June 2, 1970 |
Current U.S.
Class: |
315/3; 333/156;
313/427 |
Current CPC
Class: |
H01J
31/121 (20130101); H01J 29/708 (20130101) |
Current International
Class: |
H01J
31/12 (20060101); H01J 29/70 (20060101); H01j
023/16 (); H01j 029/46 (); H01j 029/70 () |
Field of
Search: |
;315/3 ;333/31R |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Segal; Robert
Claims
What is claimed is:
1. A cathode-ray tube oscilloscope for tracking ultrashort pulses,
comprising source means having an anode, a cathode and a grid for
producing a beam of electrons, means for focusing said beam of
electrons for transporting the same along a longitudinally
extending axis, means for producing light from said focused beam
along said axis, and deflecting means for deflecting said focused
beam from said axis a distance corresponding to an ultrashort input
signal for providing a reference time scale for the continuous time
calibration of said input signal from the light produced from said
focused electron beam relative to said axis, said deflecting means
having a serpentine-shaped transmission line formed with narrow and
curving neck portions of continuously variable width and cross
section that connect continuous equally spaced straight sections
transverse to said longitudinally extending axis by curving around
the turns of said serpentine-shaped transmission line to provide a
uniform low impedance between the ends of said transmission line
along its entire length.
2. The invention of claim 1 in which said serpentine-shaped
transmission line has spaced apart insulators along the entire
length thereof on both sides of said transmission line for rigidly
mounting the same in said cathode ray tube oscilloscope.
3. The invention of claim 1 having an anode forming an aperture and
a protrusion extending toward said grid for receiving and
collimating said electrons in a high-density beam.
4. The invention of claim 3 in which said protrusion produces a
convergent effect on said electron beam.
5. The invention of claim 1 in which said deflecting means forms
spaced apart serpentine-shaped transmission lines that are arranged
in space to form a mirror image of each other on either side of
said axis for push-pull operation by pulses that are 180.degree.
out of phase and in step with the electrons in said beam.
Description
BACKGROUND OF THE INVENTION
Fast cathode-ray tubes are required for a wide variety of
industrial and research applications. In the digital-communication
and research fields, for example, real-time cathode-ray tubes and
oscilloscopes are required that can handle input signals in the
range up to at least 50 to 250 MHz, as described in Electronics,
July 7, 1969 p. 90 et seq., by Alan J. DeVilbiss. Stated another
way, there are many and varied applications that require
cathode-ray tubes and oscilloscopes that have the ability to track,
determine, and/or record known and unknown, fast real-time input
signals, such as pulses with rise times in the range of a few
nanoseconds or less.
One fast response cathode-ray tube, hereinafter referred to as a
CRT, provides at least one planar, conductive strip means folded
into a serpentine configuration. Successively predetermined
portions of the serpentine configuration are disposed adjacent to,
but spaced from one another along the direction of an electron
stream, whereby the electron stream passes each portion in sequence
for deflections corresponding to an unknown input signal. Such a
system is described in U.S. Pat. No. 3,280,361, by Goldberg et al.,
and assigned to the EG & G Co., but as described in this
patent, the dielectric material used for mounting is attached to
the end portions of the serpentine shaped conductive strip means.
Thus, this CRT structure lacks rigidity or involves difficult
fabrication problems. Moreover, as mentioned in this patent, the
impedance matching of the structure thereof is limited since even
the end mounted dielectric material thereof may change the
impedance of the serpentine strip means. It is additionally
advantageous to provide high-electron beam densities in a CRT.
SUMMARY OF THE INVENTION
This invention, which was made in the course of, or under a
contract with the United States Atomic Energy Commission, comprises
improved CRT structures having rigidly mounted, impedance matched
serpentine traveling wave deflection means, which are improvements
over the serpentine structure of the above-mentioned patent. To
this end, in one embodiment, the serpentine structure of this
invention is supported along one whole side thereof and shaped with
narrow neck portions for providing a uniform impedance along the
overall length thereof. In accordance with further aspects of this
invention, push-pull, and mirror image-spaced apart, serpentine
conductive strips are provided. It is also an object of this
invention to provide improved fabrication means, comprising a
modular sectionalized structure and ceramic lead-ins for providing
an accurate low-distortion, fast response time, low-reject rate,
adjustably fabricated, easy to assemble CRT. In accordance with a
still further feature, this invention provides a high density
electron beam.
The above and further novel features and objects of this invention
will appear more fully from the following detailed description of
one embodiment when the same is read in connection with the
accompanying drawings, and the novel features will be particularly
pointed out in the appended claims.
BRIEF DESCRIPTION OF THE DRAWINGS
In the drawings where like elements have like reference
numbers:
FIG. 1 is a partial, extended view of one embodiment of the CRT of
this invention:
FIG. 2 is a partial cross section of the Rossi and sweep plate
section of FIG. 1 through II--II;
FIG. 3 is a partial cross section of the signal section assembly of
FIG. 1 through III--III;
FIG. 4 is a partial cross section of the electrostatic lens section
assembly of FIG. 1 through IV--IV;
FIG. 5 is a partial cross section of the marker section assembly of
FIG. 1 through V--V;
FIG. 6 is a partial cutaway view of the gun assembly of the CRT of
FIG. 1;
FIG. 7 is a partial cross section of the grid cup and first anode
electrode of FIG. 1 through VII--VII, showing the protrusion for
increasing the electron density produced by the apparatus of this
invention.
DESCRIPTION OF PREFERRED EMBODIMENT
This invention provides a fast, accurate, low distortion, high
frequency response CRT for use with a Rossi deflection of 2,200 MHz
or higher. Moreover, this invention is useful in tracking,
determining and recording fast or high speed known or unknown input
signals, such as electrical input pulses in the range from a few
nanoseconds to several picoseconds. Accordingly, this invention is
particularly useful in a wide range of scientific research
applications. However, as will be understood in more detail from
the following and also by one skilled in the art of CRT's and
oscilloscopes, this invention is useful in any of a wide variety of
industrial or research applications involving fast or high
frequency CRT input signals, and/or fast writing time, high
frequency Rossi deflections or high frequency CRT response
times.
In understanding this invention, reference is made to FIG. 1, which
illustrates one embodiment of the CRT 11 of this invention. A
source 13 produces a spray 15 of electrons 17 with velocity v, and
these electrons are formed into a suitable small diameter beam 19
that accurately passes through suitable focusing and deflecting
means, comprising deflecting stations 21, and impinges against a
conventional phosphorescent screen 23 at one end of a glass
cylinder 25. For properly transporting the beam and impacting it
against the screen 23, the CRT 11 advantageously comprises an
evacuated electron gun assembly 27, a marker deflection structure
29, an electrostatic lens section 31, although a magnetic lens may
alternately be used, a signal deflection structure 33, a high
frequency timing and Rossi linear sweep plate means 35, and an
evacuated glass cylinder 25 having helical conductor means 37
around the circumference thereof.
It will be understood from the above, that CRT 11 involves
complicated and accurately located structures involving stringent
standards and requirements. In this regard, the CRT 11 of this
invention meets the difficult assembly and high frequency operating
requirements involved in industrial and research uses, and
overcomes the high-rejection rates known heretofore. To this end
the CRT 11 employs a modular design and assembly system that
permits physical adjustment and testing of the various parts
thereof, and which overcomes or lessens the expensive problems of
assembling these parts on a single frame of rods, as was done
heretofore.
As shown in FIG. 1, modules 39 which sequentially form the stations
21 for assembly between gun 27 and screen 23, comprise round cross
section tubes 41 and square cross section tubes 43, each of which
is made of metal and carries round, disc shaped flanges 45 having
oppositely mating cylindrical shoulders or niches for coaxial
alignment along a single x axis passing azimuthally through and
along the center of the modules 39 formed by the round and square
cross section tubes. Also, appropriate aperture discs 47 are
arranged and heliarc welded between modules 39.
The described modular design is based on the approach of building
the deflection structures of stations 21 into the individual
modules 39 of the body 49 of CRT 11, and the precise complete
mechanical assembly adjustment and critical testing of the
individual components of each module 39 before the assembly
thereof. The individuals modules 39 of CRT 11 are then joined
together by heliarc welds 51 to form the complete CRT 11. As
described in more detail hereinafter, the gun 27 and front bulb or
screen cylinder 25 are also built as individual sections and joined
to the deflection station modules 39 by heliarc welds 51. Likewise,
the modular design of CRT 11, has the advantage of ease and economy
of assembly while consistently meeting stringent specifications
with a low-rejection rate, and without constraints being imposed to
compromise the design of CRT 11 for the sake of compatibility with
existing equipment and power supplies.
Additionally, this modular assembly of CRT 11 permits completion
and final assembly of coaxial lead-ins 53, which permit the
mentioned critical tests to be performed. These coaxial lead-ins 53
have ceramic-to-metal vacuum seals 55 designed for both 50 ohm GR
connectors and 100 ohm GR connectors. Also, lead-ins 53 provide the
correct impedance within 1 ohm for the 50 ohm connectors, and
within 3 ohms for the 100 ohm connectors. These seals 55 have the
advantage of reliability and vacuum integrity. In this regard also,
the sectionalized, tubes 43 permit easy and vacuumtight location
and assembly of the coaxial, ceramic, lead-ins 53, which have
conductor pins 57 and thin discs 59 of molybdenum for securing the
vacuumtight seals 55 between the pins 57 and coaxial ceramic
elements 59'.
Basically, the final vacuum seal has been separated from the
electrical connections by the described modules 39 of CRT 11.
Moreover, the described ready access provided at the ends of the
individual modules 39 and the complete inspection and adjustment
thereof, permits the individual subassembly of modules 39 in lot
quantities. Thus, the final assembly of CRT 11 joins the several
main subassemblies after they have been completely checked out and
inspected, whereby rejects are caught at an early stage in the
assembly and repairs of the parts of modules 39 represent a minor
problem.
Another advantage of the described modules 39, comprises the
exhaust tubulation 61 (shown in FIG. 1 and FIG. 6), and a cold weld
63 with an annealed copper tubing 65. A pinch-off 67, is also
provided. In this regard, this pinch-off 67 has proven to be very
reliable in actual production and use, since it has the advantage
that no heat is used during the pinch-off process to a degradation
of the vacuum in CRT 11.
The described modular assembly system of this invention is also
advantageous in the accurate assembly, testing and adjustment of
the traveling-wave deflection structures 69 of the deflection
stations 21 of this invention. Referring to FIG. 2, for example,
the serpentine shaped, traveling-wave, delay-line structure 69 of
Rossi, sweep plate deflector 35, is rigidly mounted along both
edges 71 of the delay line structure 69 in grooves 73 in spaced
apart insulators 75 and brazed to the insulators 75. Moreover, by
means of careful assembly and spring contacts 77 for the electrical
connections 79 of lead-ins 53, which is all made possible by the
described modular design of this invention, the spacings,
alignment, and electrical characteristics of these elements are
maintained within a few thousands of an inch or less.
This invention is also advantageous since it provides a
serpentine-shaped, traveling-wave, delay-line, deflection
structures 69 that has the desired impedance. Referring to FIG. 3,
for example, signal deflector 33 has a serpentine-shaped,
traveling-wave, delay-line, charged particle (electron) deflection
structure 69 that is photoetched from a uniform thickness plate
having little or nil magnetism properties, and a cross section
formed to provide the desired impedance when rigidly mounted and
assembled in insulators 75 on both edges 71 thereof. To this end,
as shown in FIG. 3, the assembled serpentine deflection structure
69 has a variable cross section that is uniformly adjusted to be 50
or 100 ohms, which is checked by a high-resolution TDR along its
length. This particular, described serpentine structure 69 thus
gives a unique narrow cross section around the serpentine turns.
This provides high frequency, undistorted response, thereby to
insure that the electron beam 19 is in step with the voltage signal
e.g., an unknown pulse) impressed on this variable cross section,
serpentine structure 69 & is synchronous therewith in phase.
Thus, this (unknown) signal can be compared accurately with a high
frequency sine reference wave signal, e.g., in the opposite
direction. Moreover, this specific serpentine structure 69 having
the described balanced, uniform impedance along its length,
provides the particular advantage of sensitivity, whereby the beam
scan, i.e., how far the beam 19 can be deflected without
distortion, is increased. Additionally, the writing speed is
increased, faster input or unknown signals can be tracked, and
resonant, higher frequency Rossi deflection signals can be employed
without distortion.
Still further, a uniform easily adjustable spacing between
parallel, periodic, "turns" 81 of the serpentine structure 69 is
provided, these spacings can be wider, more closely controlled in
accordance with CRT 11 design and impedance matching requirements
of the allied equipment without any constraints being imposed to
comprise the tube design for the sake of compatibility with
existing equipment and power supplies, the serpentine structure 69
can be longer, the power requirements are less, and low-stray
capacitance is provided consistently and reproducibly in production
quantities.
Advantageously, each serpentine structure 69, comprises a
molybdenum delay line uniformly about 10 mils thick. However, this
thickness dimension may be up to 20 mils. Also, the ends 83 curve
for a rigid attachment to connections 79, while the edges 71 are
brazed to ceramic insulators 75 by metallizing i.e., with solder
fill.
The system of this invention has the further advantage that
two-spaced apart, parallel serpentine delay-line structures 69 can
be adjustably assembled in deflector 33 for 10-20 volt, 0-2,000 MHz
signals, and these signals can be 180.degree. out of phase in the
two respective serpentine structures 69 for balanced push-pull
operation. To this end, these two serpentine structures can be
assembled, and are advantageously mirror images of each other in
accordance with the accurate sectionalized and adjustable assembly
system of the modules 39 of this invention.
The round cross section tubes 41 of modules 39 have the added
advantage of spacing the walls thereof far from the structure
assembled therein. Thus, the impedance of the serpentine signal
deflector 33 is easily assembled, tested, and controlled in a
rigid, shockproof subchassis.
Referring to FIG. 4, the lens 31, which is likewise assembled with
similar advantages in a round cross section tube 41, utilizes a
mechanical mount that provides precise centering of the through
coaxial lens elements 85 with respect to the electron beam within a
few mils. The lens 31, which is advantageously an electrostatic
lens, also incorporates an adjustment feature precisely to
orientate the ends 87 of the lens elements 85 in lens 31
perpendicular to the axis of the electron beam 19. This adjustment
is accomplished by using two micrometer heads to provide the tilt
adjustment in the vertical and the horizontal plane. After this
alignment procedure, which also comprises clamping the lens
elements 85 and lens 31 relatively in place, the micrometer heads
are removed. In this regard the described modular design permits
the testing, adjustment and assembly of interchangeable lenses 31.
For this adjustment procedure, the effect of the electron beam is
advantageously used as an indication for the proper lens alignment
whereby the lens 31 is perpendicular to the electron beam 19 within
1/2.degree. or less.
Referring to FIG. 5, the structure in the square-cross section tube
of the marker 29, on the other hand, requires less spacing.
Additionally this square-cross section permits the lead-ins 53 to
be off center to line up with the widely spaced ends 83 of the
closely spaced, periodic, "turns" 81 of the serpentine structure 91
of this marker 29.
The electron source 13, which is illustrated in FIG. 6, is a
negative-grid, high-density beam, gun 27 having a beam collimating
and electrical field curving anode electrode 97 which forms an
annular protrusion 99 at the input end 101 of flat plate 103. This
gun 27 differs from conventional structures in that the protrusion
99 forms a sleeve around the beam 19 toward grid 105 as shown in
FIG. 7. Compared to conventional anodes, the anode electrode 97 of
this invention increases the electron beam current by a factor of
1.8 or more on production quantities of tubes 11.
The effect of the protruding sleeve formed by protrusion 99 is to
change the curvature of equipotentials 107 in accelerating region
109 of electron gun 27. This change in the curvature is such that
electric field 111 produced by the cathode-anode structure 113 is
modified to have a convergent effect on the electron beam 19,
rather than a divergent effect experienced by a plain aperture 115
in a flat plate 103 without a protrusion 99. The above-described
convergent effect illustrated by dashed lines 117, provides a
higher electron beam current passing through the limiting aperture
115.
Advantageously, the connections 119 of the electron gun 27, which
is illustrated in FIG. 6, have a potting compound 121 that insures
the reliability of the connections and resistance to arcing,
thereby reliably maintaining the same under severe environmental
conditions of shock, vibration, humidity, dirt or dust.
To insure that the CRT 11 maintains a high-vacuum under usage and
long shelf life, the parts thereof receive an extensive high-vacuum
processing cycle. To this end, all the metal parts undergo a
1,000.degree. C. high-vacuum firing for 1 hour prior to assembly to
outgas the parts. After the assembly process, the completed section
is subjected to a 450.degree. C. vacuum bakeout. Prior to assembly,
the glass bulb of cylinder 25, which is illustrated in FIG. 1, with
the phosphor screen 23 and an aquadag resistive spiral 37 with a
chrome oxide resistive coating has a 380.degree. vacuum bakeout for
1 hour. This bakeout removes a large part of the evolved gaseous
products from the assembly of cylinder 25 and the whole bulb
assembly 125.
After this vacuum bakeout of the bulb assembly 125, the CRT 11 is
assembled and the entire CRT undergoes a 380.degree. C. bakeout
during the 8-hour exhaust and vacuum processing cycle. This
extensive exhaust and vacuum processing cycle has been a major
factor in achieving uniformly high-emission current from the
cathode 127 and in achieving long-life in production quantities of
CRT 11.
In one example for the above-described assembly cycle, the tubes 41
and 43 and the flanges 45 therefor are assembled, vacuum brazed in
a furnace and leak checked. Finish machining of flanges 45 then
provides concentric diameters and shoulders for both flanged ends
131 of each respective tube 41 and 43. To this end a mandrel in one
end 131 provides for machining both ends to provide flat ends 131
to 1 mil having a 32 micron finish, and concentricity to 1 mil.
An assembly jig then registers on each of the respective machined
shoulders of the flanged tubes 41 and 43 and spot welding
accurately places the internal elements 133 therein. Also the
lead-ins 53 are assembled in tubes 41 and 43 respectively, heliarc
welded in place, and connected to the internal elements 133.
Thereafter, these lead-ins 53 and internal elements 133 are
electrically checked and adjusted, e.g., with time domain
reflectometers for adjusting the impedances thereof for minimum
reflectance.
The completed modules 39 are individually vacuum baked at
1,000.degree. C., assembled in line with their shoulders 135 in
ends 131 mating with each other, and heliarc welded. Leak checking
of this assembly then prepares for pump out, bakeout at 400.degree.
C., metal pinch-off, etc.
Advantageously, fiducial marks 137 and the serial number of CRT 11
are abraded onto the internal surface of the glass faceplate 129.
These fiducial marks serve the purpose of increasing the precision
of the recovery and analysis of the recorded data. These fiducial
marks provide a fixed reference on the face of CRT 11 to obtain
increased precision when correlating calibration films with the
recorded data.
In one example for producing these fiducial marks 137, the marks
137 and the patterns thereof are first cut into a thin metal mask
by photoetching. The pattern is transferred to the internal surface
of the glass by an abrasive process of blowing an abrasive onto the
glass on which the mask has been cemented.
To this end the metal mask is cut from 3 mil stock, the fiducial
marks are photoetched into the mask, cement attaches the mask to
the inside of face 139, an eraser removes the excess cement, and an
air driven abrasive abraids the glass.
Controlled illumination of the fiducial marks 137 is provided by
edge lighting with an electroluminescent tape around the edge of
the face 139 of bulb assembly 125. The electroluminescent tape is
held in position by being molded into a sleeve of insulating
material (not shown) in which the high-voltage lead is also molded.
Better illumination has been obtained without any intermediate
material between the electroluminescent tape and the glass of bulb
assembly 125 than clear plastic or cement.
The described CRT 11 provides an oscilloscope having many
advantageous performance and assembly features. In terms of
sensitivity in volts per trace width, scan in trace widths, writing
speed in trace widths per second and bandwidth, the described
high-density electron beam 19, vacuumtight lead-ins, specific,
variable cross section serpentine structure 69, and the described
modular assembly system provides superior results for ultrashort
and high frequency pulsework, without sacrificing other operating
characteristics even with existing auxiliary equipment and existing
CRT design requirements. The low, controlled, uniform impedances
and low-stray capacitances are specifically and actually provided
for long periodic serpentine structures having wide spacing between
the "turns" 81 thereof. Also, the described system of this
invention, provides an accurate, rigid, shockproof, insulated
assembly in round and square cross section modules 39 that are
bakedout, leak-checked, and electrically tested, and selectively
adjusted to provide long-operating lifetime, high-performance, and
low-reject rates in production quantities. In actual practice
low-stray capacitances of 0.4 .mu..mu.f are provided at 100 ohm
levels for signal rise times of 10.sup.-.sup.10 seconds or less.
Other actual parameters achieved with this invention, comprise 0.50
ns. maximum transmission rise times, 4.+-.0.2 ns. transit times,
50.+-.2.OMEGA. marker serpentine structures, Rossi systems with
VSWR of 1.4, beam currents with dynamic cutoff of 200 v. above
static and static cutoff of 350 v..+-.50 v.
* * * * *