Irradiating filament and method of making same

Information

  • Patent Grant
  • 6146322
  • Patent Number
    6,146,322
  • Date Filed
    Wednesday, October 30, 1996
    28 years ago
  • Date Issued
    Tuesday, November 14, 2000
    24 years ago
Abstract
A filament for irradiating a living body has a core material capable of irradiating radioactive radiation clad in a tubular casing of protective material different from the material forming the core. The materials forming the core and casing have a purity not less than 99.5 atomic percent and a grain size not exceeding 30 .mu.m and the outer diameter of the filament is not less than 80 .mu.m.
Description

BACKGROUND OF THE INVENTION
This invention relates to a filament for irradiating a living body, comprising a core of material capable of irradiating radioactive radiation after activation, the core being clad in a casing of protective material, wherein the materials forming the core and casing differ from one another.
The invention also relates to a method for producing a filament for irradiating a living body.
Endoluminal brachytherapy, and more particularly percutaneous transluminal brachytherapy, currently face difficulties for handling the radioactive material, either on a therapeutical viewpoint or on a manufacturing viewpoint. As a matter of fact, it is quite frequent that the structure embodying the radioactive material is bulky and lacks flexibility, whereby the material is difficult to operate through tortuous vessel configurations or narrow passages thereof; this may cause damage or even destruction of the radioactive structure together with the resulting risk of harmful influence on the organism. Furthermore, the radioactive material may enter into direct contact with the vessel walls, which greatly amplifies the risk of unwanted damage to the vessel. And when the radioactive material is merely coated or covered by an outer material, the coating or cover may help protecting the vessel wall from direct contact with the radioactive source, but there is still a substantial danger of having the radioactive material or particles thereof entering into unwanted contact with the vessel wall in case of deterioration of the coating or cover or because the coating or cover still have uncontrolled pores through which the radioactive material may cause damage to the vessel.
For example, the document WO 93/04735 describes an apparatus for the treatment of an artery, comprising a radioactive dose and means operatively connected to such a dose to bring it into a selected region of an artery. In one embodiment, the apparatus comprises a wire wound sheath removably positioned over a windowed housing made of a wire winding containing a radioactive dose, whereby relative motion between the sheath and housing permits moving the windowed housing in and out of the sheath to expose the radioactive dose in some place of an artery. In another embodiment the apparatus comprises a motion wire having a radioactive dose affixed at its distal end and a retractable sheath formed of a helically wound member positioned over the motion wire and radioactive configuration to provide a measure of shielding to the radioactive dose during insertion and removal of the system into an artery, whereby the sheath may be retracted to expose the radioactive dose at a selected place in the artery. A further embodiment comprises a shaft portion having at its distal end a canister containing a radioactive dose and provided with a remotely actuated window which can be manipulated to expose the radioactive dose in an injured area of an artery. In a still further embodiment, a plurality of radioactive dose means are encased in a heat shrinkable polymer catheter tip having spacers made of a meltable material to provide encapsulation of the radioactive dose means, which provides flexibility of the apparatus but not longitudinal homogeneity of the radioactive source. In a balloon configuration of the apparatus, radioactive elements are affixed to the outer surface of an angioplasty balloon. In a stent arrangement of the apparatus, the radioactive element may be associated with an expandable stent and it is the radioactive means that may be included in the stent as a cladding, a coating, or an additive within the basic stent material, or an attachment by other means to the stent.
As a further example of the aforesaid drawbacks, U.S. Pat. No. 5,059,166 describes an intra-arterial stent with the capability to inhibit intimal hyperplasia by means of radioactive radiation. The document refers to a radioisotope integral to an arterial stent which can irradiate the tissue in close proximity to the implantation site of the stent. In one embodiment, a helical coil spring stent is fabricated from a pure metal or alloy which has been activated so that it has become radioactive, i.e., it is a radioisotope; the radioisotope used for this purpose may be an alpha, beta, or gamma emitter, a beta emitter such as Vanadium 48 being preferred because of its short travel in human tissue and 16 days half-life and only 8% of emitted energy from gamma radiation. In another configuration, the stent spring wire is made from a metal such as steel into which is alloyed an element that can be made into a radioisotope, for example Phosphorus 32 which is a 14.3 day half-life beta emitter. In a further configuration, the stent wire is made from a radioisotope core material with an outer covering that has the attributes that are desirable for being a coil spring. In a variant, the stent wire is made of a radioisotope coating plated onto a spring material core. Still a further embodiment shows a more complex configuration in which a core of some material suited for stents is plated with a radioisotope coating which is in turn coated with an anti-thrombogenic coating such as carbon.
Within the frame of a centering configuration aimed at uniformly applying a radioactive radiation to a vessel wall, the document EP 0633041 A1 outlines the use of a radioactive emitter in the form of a filament of small diameter, which may be coiled. Filament technology has the advantage of a dense concentration of the radioactive dose in a small volume of the source allowing a reduced diameter and a better maneuverability in narrow and/or tortuous vessels. In one embodiment, the filament may be made of 89 Yttrium heat elaborated under vacuum to a diameter equal to or less than 0.2 mm.
In the environment of a medical appliance for the treatment of body vessels by ionizing radiation described in EP 0 686 342 A1, published Dec. 13, 1995, the filament technology is enhanced by having a filament, which may be in the form of a coil, coated by a neutral material such as Titanium.
Clad composite filaments are generally shown in WO 94/16646 and WO 95/30384.
All documents cited herein, including the foregoing, are incorporated herein by reference in their entireties for all purposes.
It is an object of this invention to improve the conditions of use in a patient as well as those of handling the sources used for irradiating a living body and more particularly those sources used for endoluminal or percutaneous transluminal brachytherapy. It is a further object of the invention to improve such conditions by means of a filament which is highly safe.
Still a further object of the invention is a method for manufacturing a filament for irradiating a living body which is fully controllable, devoid of hazardous technological operations with radioactive substances, and which results in a product which practically eliminates the risk of having radioactive core materials or particles thereof entering into unwanted contact with a living body.
SUMMARY OF THE INVENTION
Accordingly, with the materials forming the core and protective casing having a grain size equal to or less than 30 .mu.m, a filament is achieved which has all the advantages of the filament technology for dense concentration of radioactive dose and for exceptional flexibility and maneuverability through narrow and/or tortuous areas of body vessels. And this is achieved within a configuration in which the core and casing have a great homogeneity which strongly reduces brittleness of the materials and which practically eliminates any risk of having cracks or ruptures in case of deformation as well as any risk of having radioactive particles wandering through uncontrolled pores of the protective casing. Safe handling of the radioactive core is thus highly effective and there is no danger of unwanted harmful influence of the radioactive material on the organism.
Where the materials forming the core and protective casing have a grain size equal to or less than 10 .mu.m, the filament achieves a further degree in terms of isotropic lateral flexibility and homogeneous distribution of the core material throughout the length of the filament, with a further safety in terms of brittleness reduction of the materials.
Where the materials forming the core and protective casing have a purity of at least 99.5 atomic percent, homogeneity of the filament is still enhanced with the corresponding safety and absence of brittleness. And when the material forming the core is alloyed by 0.1 to 0.3 atomic percent with the material forming the protective casing and the material forming the protective casing is alloyed by 0.1 to 0.3 atomic percent with the material forming the core, the strength of the filament is still strongly increased without any loss on the control of the tightness of the materials; the probability of cracks or damage to the assembly is further reduced. With a filament having an outer diameter equal to or over 80 .mu.m a limit is achieved on the strength of the materials while retaining the aforesaid qualities; a filament of that size is specifically suitable for percutaneous transluminal procedures. With the materials forming the core and protective casing having the same crystal lattice, which may be advantageously a hexagonal crystal lattice, high purity and small grain size as well as the mechanical properties and pore control of the assembly are further enhanced.
Preferably, the material forming the core is a beta radiation emitter, and more particularly Yttrium or Thulium, to take advantage of an appreciable irradiation combined to a suitable half-life. This is desirable to allow procedure times that are manageable in interventional medicine such as percutaneous transluminal angioplasty. Moreover, beta emitters such as Yttrium or Thulium have a hexagonal crystal lattice which best fits to the employed casing material. Still preferably, the material forming the protective casing is Titanium, which has a short half-life and which is biocompatible while having very good mechanical properties providing absence of leakage of the core material. Moreover, the hexagonal crystal lattice of Titanium provides compatible deformation properties with the core materials.
The filament may be easily coiled to still further promote the elasticity of the resulting source in case of handling through tortuous vessels without the risk of damage or cracks in the assembly.
By the steps of forming an initial billet of core material capable to irradiate radioactive radiation after activation, forming an initial tubular preform of casing material differing from the core material, working the initial billet and tubular preform until they have a grain size equal to or less than 30 .mu.m, inserting the billet into the tubular preform to have an assembly, drawing the assembly through a series of successive dies of decreasing size with intermediate annealing of the assembly in intervals between successive dies until the assembly has a final outer diameter, and end sealing of the casing material on the core material, a method for producing a filament is achieved which is fully controllable, allowing decrease of the internal stress and grain size of both the core and casing materials. Each draw sequence through a die reduces the grain size by fragmentation of the grains and the further re-crystallization occurring during the intermediate annealing between successive dies starts a re-crystallization at the reduced grain size. Growth of the grain is thus avoided; a 10 .mu.m grain size may be securely achieved and from that basis it is readily possible to obtain a 5 to 7 .mu.m grain size without any risk of uncontrolled growth of the grain size. Final sealing of the casing material on the core material may be made without affecting the structure of the materials. The resulting filament has thus a high homogeneity which reduces its brittleness and avoids the risk of having cracks or ruptures therein under current deformation. The risk of having unwanted radioactive particles wandering through uncontrolled pores of the filament is practically eliminated.
By the aforesaid method, the assembly comprising casing and core materials may be drawn up to an outer diameter equal to or over 80 .mu.m without affecting the strength of the materials and qualities of the filament. And the method may comprise the step of coiling the drawn assembly before end sealing of the casing material on the core material, still without affecting their homogeneity and without any risk of cracks or ruptures in the filament.
When the method includes the step of cutting the drawn assembly into a plurality of sub-assemblies before end sealing of the casing material on the core material, whereas end sealing of the casing material on the core material is made on each of the sub-assemblies, filament assemblies may be produced economically in a continuous manner, the assemblies being then cut at will.
Advantageously, end sealing of the casing material on the core material is made by laser welding for a precise procedure.
When the core material and the protective casing material have a purity of at least 99.5 atomic percent, the method still achieves a greater homogeneity for the resulting filament under the same basics of fully controlled manufacture. And to enhance the mechanical properties of the filament while further reducing the probability of cracks or damage, the method may comprise the preliminary step of alloying the core material by 0.1 to 0.3 atomic percent with the casing material and alloying the casing material by 0.1 to 0.3 atomic percent with the core material.
To further enhance the technological feasibility of the process the core material and casing material may have the same crystal lattice, preferably a hexagonal crystal lattice which will fit best with compatible strength, plasticity and annealing temperatures.
When the method further comprises the step of activating the core material in the casing material in a nuclear reactor, activation is made at the final stage of production of the filament, which is easier and substantially reduces the manipulations of radioactive filament. The resulting cost is lower and the risks of contamination are strongly limited.
In sum, the present invention relates to a filament having a core of material capable of irradiating radioactive radiation after activation. The core is clad in a casing of protective material and the materials forming the core and casing differ from one another and have a grain size equal to or less than 30 .mu.m. The filament materials forming the core and protective casing may have a grain size equal to or less than 10 .mu.m. The core and protective casing may have a purity of at least 99.5 atomic percent. The core may be alloyed by 0.1 to 0.3 atomic percent with the material forming the protective casing, and the material forming the protective casing may be alloyed by 0.1 to 0.3 atomic percent with the material forming the core. The filament may have an outer diameter equal to or over 80 .mu.m. Also, the filament may form a coil. The core and protective casing may have the same crystal lattice, a hexagonal crystal lattice, or a cubic crystal lattice. The core may be a beta radiation emitter. The material forming the core may be Yttrium, Thulium, Europium, Gadolinium, Terbium, Iridium, or Cesium. The material forming the protective casing may be Titanium, Platinum, Silver, or Gold.
A first material may be adapted to emit radiation and a second material may cover the first material and the first and second material each may have a grain size equal to or less than about 30 .mu.m.
The invention also relates to a method for producing a filament which includes forming an initial billet of core material capable of irradiating radioactive radiation after activation, forming an initial tubular preform of casing material differing from the core material, working the initial billet and tubular preform until they have a grain size equal to or less than 30 .mu.m, inserting the billet into the tubular preform to form an assembly, drawing the assembly through a series of successive dies of decreasing size with intermediate annealing of the assembly and intervals between successive dies until the assembly has a final outer diameter, and sealing the casing material on the core material. The method may include a step where: the final outer diameter is equal to or over 80 .mu.m; the drawn assembly is coiled before end sealing of the casing material on the core material; the drawn assembly is cut into a plurality of sub-assemblies before end sealing of the casing material on the core material, and end sealing of the casing material on the core material is made on each of the sub-assemblies; end sealing of the casing material on the core material is made by spot laser welding; the core material and the protective casing material have a purity of at least 99.5 atomic percent; the core material is alloyed by 0.1 to 0.3 atomic percent with the casing material and the casing material is alloyed by 0.1 to 0.3 atomic percent with the core material; the core material and the casing material have the same crystal lattice or a hexagonal crystal lattice; the core material is a beta radiation emitter; the core material is Yttrium or Thulium; the casing material is Titanium; activation of the core material in the casing material is in a nuclear reactor.
Another method for producing an irradiating filament includes providing a first material that emits radiation and providing a second material, working the first and second materials until each respective material has a grain size equal to or less than about 30 .mu.m, disposing the first material within the second material to form a composite assembly having a first end and a second end, and drawing the composite assembly through a series of successively smaller dies and annealing the composite assembly. The method may include steps of covering and sealing the first end and second end with the second material.
These and other objects and features of the invention will become readily apparent from the following detailed description with reference to the accompanying drawings which illustrate, diagrammatically and by way of example only, two embodiments of a filament according to the invention.





BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is an axial cut of a filament according to the first embodiment;
FIG. 2 is a cross section according to line I--I of FIG. 1; and
FIG. 3 is an axial view, partly cut, of a radiation source formed of a coiled filament according to the second embodiment.





DETAILED DESCRIPTION
The filament 1 shown in FIG. 1 comprises a core 2 of material capable of irradiating radioactive radiation. Preferably, the core 2 is made of a cylindrical wire of a beta radiation emitter such as Yttrium or Thulium having a purity of 99.5 atomic percent. Yttrium and Thulium both have a hexagonal crystal lattice and a relatively small grain size.
The core 2 is clad in a tubular casing 3 of protective material different from the material of the core 2. Preferably, the casing 3 is made of Titanium having a purity of 99.5 atomic percent, preferably 99.9 atomic percent. Titanium also has a hexagonal crystal lattice with a relatively small grain size.
The materials, Yttrium and Thulium, forming the core 2, and Titanium, forming the protective casing 3, have a grain size not exceeding 30 .mu.m, preferably equal to or less than 10 .mu.m. The outer diameter D of the filament 1 is not less than 80 .mu.m.
Advantageously, the production of the filament 1 may be obtained by forming an initial billet of core material and an initial tubular preform of casing material differing from the core material. Such billet and tubular preform are worked, for instance by deformation and thermal treatment or as ingots and serial consequent hot drawing, until they have a grain size equal to or less than 30 .mu.m. The billet is then inserted into the tubular preform to form an assembly which is drawn through a series of successive dies of decreasing size. In intervals between successive dies, the drawn assembly is allowed to anneal, which process provides a decrease in internal stress and allows formation of a small grain structure of the core and casing materials less than 30 .mu.m. The casing is then hermetically sealed on the core 2, preferably by taking off by etching a portion of the Yttrium or Thulium wire at its ends 4, and thereafter closing the ends 5 of the Titanium tube 3 into a smooth spherical tip which does not substantially exceed the outer surface at the filament 1. For example, this procedure may be achieved by means of spot laser welding. After completion of this assembly, the filament may be brought into a nuclear reactor (not shown) for activation of the core 2 in the casing 3.
According to a variant, the material forming the core 2 may be alloyed by 0.1 to 0.3 atomic percent of the material forming the casing 3 with the material forming the casing 3 alloyed by 0.1 to 0.3 atomic percent of the material forming the core 2. The manufacturing process follows then as described hereabove.
The filament 6 shown in FIG. 3 is made identically as and with the same integers (bearing the same reference numerals) as the filament 1 of FIG. 1 or its alloyed variant. After completion of the assembly of core 2 and casing 3, the filament 6 is applied on a mandrel (not shown) in order to be formed as a coil 7 and then end sealing of the casing material on the core material is made as described hereabove. After completion of the assembly forming the filament 6 and its coil shaping 7 and sealing, the filament may be brought into a nuclear reactor for activation of the core 2 in the casing 3.
Variants are available. For instance, instead of Yttrium or Thulium, other emitters may be used for the core, more particularly Europium or Gadolinium or Terbium which also have a hexagonal crystal lattice. It is also possible to use other metals such as Platinum or Gold or Silver instead of Titanium for forming the casing 3, although such metals have a cubical crystal lattice. Such potential coverage materials could be preferably used with Iridium, Cesium or other core materials having a cubic crystal lattice.
The filament 1 as shown in FIGS. 1 and 2 may be used as such or affixed at the end of a guiding structure or of a guide wire as used in endoluminal or transluminal brachytherapy, or as a wire to partly or completely form or make part of a stent, in which case energization in the nuclear reactor will be made after completion of the stent structure.
It will be evident from considerations of the foregoing that the irradiating filament is now available and may be constructed using a number of methods, in a wide variety of sizes and styles for the greater efficiency and convenience of a user.
The above described embodiments of the invention are merely descriptive of its principles and are not to be considered limiting. Further modifications of the invention herein disclosed will occur to those skilled in the respective arts and all such modifications are deemed to be within the scope of the invention as defined by the following claims.
Claims
  • 1. A filament for irradiating a living body, comprising a core of radiation emitting material, the core being clad in a casing of protective material, wherein the materials forming the core and casing differ from one another and the materials forming the core and protective casing have a grain size equal to or less than 30 .mu.m.
  • 2. A filament according to claim 1, wherein the materials forming the core and protective casing have a grain size equal to or less than 10 .mu.m.
  • 3. A filament according to claim 1, wherein the materials forming the core and protective casing have a purity of at least 99.5 atomic percent.
  • 4. A filament according to claim 1, wherein the material forming the core is alloyed by 0.1 to 0.3 atomic percent with the material forming the protective casing, and the material forming the protective casing is alloyed by 0.1 to 0.3 atomic percent with the material forming the core.
  • 5. A filament according to claim 1, wherein the casing material has an outer diameter equal to or over 80 .mu.m.
  • 6. A filament according to claim 1, wherein the materials forming the core and protective casing have the same crystal lattice.
  • 7. A filament according to claim 1, wherein the materials forming the core and protective casing have a hexagonal crystal lattice.
  • 8. A filament according to claim 1, wherein the material forming the core and protective casing have a cubic crystal lattice.
  • 9. A filament according to claim 1, wherein the filament forms a coil.
  • 10. A filament according to claim 1, wherein the material forming the core is a beta radiation emitter.
  • 11. A filament according to claim 1, wherein the material forming the protective casing is selected from the group consisting of Titanium, Platinum, Silver, and Gold.
  • 12. A filament according to claim 1, wherein the material forming the core is selected from the group consisting of Yttrium, Thulium, Europium, Gadolinium, Terbium, Iridium, and Cesium.
  • 13. A filament according to claim 12, wherein the material forming the core is Yttrium.
  • 14. A filament according to claim 12, wherein the material forming the core is Thulium.
  • 15. A filament according to claim 11, wherein the material forming the protective casing is Titanium.
  • 16. An irradiating filament comprising:
  • a first material adapted to emit radiation and a second material covering the first material wherein the first and second material each have a grain size equal to or less than about 30 .mu.m.
  • 17. A clad composite filament comprising a core and a case, the core comprising a radiation emitting material and the case comprising a biocompatible material which is different than the radiation emitting material, wherein both of the radiation emitting material and the biocompatible material have a grain size which is less than or equal to 30 .mu.m.
  • 18. The filament of claim 17, wherein both of the radiation emitting material and the biocompatible material have a grain size which is less than or equal to 10 .mu.m.
  • 19. The filament of claim 17, wherein the radiation emitting material is alloyed with 0.1 to 0.3 atomic percent of the biocompatible material, and the biocompatible material is alloyed with 0.1 to 0.3 atomic percent of the radiation emitting material.
  • 20. The filament of claim 17, wherein the case has an outer diameter of at least 80 .mu.m.
  • 21. The filament of claim 17, wherein the radiation emitting material and the biocompatible material have the same crystal lattice.
  • 22. The filament of claim 17, wherein the radiation emitting material and the biocompatible material have hexagonal crystal lattices.
  • 23. The filament of claim 17, wherein the radiaton emitting material and the biocompatible material have cubic crystal lattices.
  • 24. The filament of claim 17, wherein the filament forms a coil.
  • 25. The filament of claim 17, wherein the radiation emitting material is a beta radiation emitter.
  • 26. The filament of claim 17, wherein the biocompatible material is selected from the group consisting of titanium, platinum, silver, gold, and alloys thereof.
  • 27. The filament of claim 17, wherein the radiation emitting material is selected from the group consisting of yttrium, thulium, europium, gadolinium, terbium, iridium, cesium, and alloys thereof.
  • 28. The filament of claim 27, wherein the radiation emitting material is yttrium.
  • 29. The filament of claim 27, wherein the radiation emitting material is thulium.
  • 30. The filament of claim 26, wherein the biocompatible material is titanium.
Priority Claims (1)
Number Date Country Kind
95119124 Dec 1995 EPX
US Referenced Citations (141)
Number Name Date Kind
1442051 Cummings Jan 1923
2546761 Loftus Mar 1951
2862108 Meilink Nov 1958
2955208 Stevens Oct 1960
3060924 Rush Oct 1962
3147383 Prest May 1962
3324847 Zoumboulis Jun 1967
3505991 Hellerstein et al. Apr 1970
3643096 Jeffries, Jr. et al. Feb 1972
3669093 Sauerwein et al. Jun 1972
3674006 Holmer Jul 1972
3750653 Simon Aug 1973
3811426 Culver et al. May 1974
3861380 Chassagne et al. Jan 1972
3866050 Whitfield Feb 1975
3927325 Hungate et al. Dec 1975
3970073 Greene Jul 1976
4096862 DeLuca Jun 1978
4220864 Sauerwein et al. Sep 1980
4225790 Parsons, Jr. et al. Sep 1980
4244357 Morrison Jan 1981
4281252 Parsons, Jr. et al. Jul 1981
4314157 Gaines Feb 1982
4364376 Bigham Dec 1982
4402308 Scott Sep 1983
4584991 Tokita et al. Apr 1986
4588395 Lemelson May 1986
4631415 Sauerwein et al. Dec 1986
4697575 Horowitz Oct 1987
4702228 Russell, Jr. et al. Oct 1987
4706652 Horowitz Nov 1987
4763642 Horowitz Aug 1988
4763671 Goffinet Aug 1988
4815449 Horowitz Mar 1989
4819618 Liprie Apr 1989
4851694 Rague et al. Jul 1989
4861520 van't Hooft et al. Aug 1989
4881937 van't Hooft et al. Nov 1989
4881938 van't Hooft Nov 1989
4897076 Puthawala et al. Jan 1990
4936823 Colvin et al. Jun 1990
4940452 Rohe et al. Jul 1990
4963128 Daniel et al. Oct 1990
4969863 van't Hooft et al. Nov 1990
4976266 Huffman et al. Dec 1990
4976680 Hayman et al. Dec 1990
4994013 Suthanthiran et al. Feb 1991
5030194 Van't Hooft Jul 1991
5059166 Fischell et al. Oct 1991
5069226 Yamauchi et al. Dec 1991
5084001 Van't Hooft et al. Jan 1992
5084002 Liprie Jan 1992
5092834 Bradshaw et al. Mar 1992
5092877 Pinchuk Mar 1992
5103395 Spako et al. Apr 1992
5106360 Ishiwara et al. Apr 1992
5120973 Rohe et al. Jun 1992
5139473 Bradshaw et al. Aug 1992
5141487 Liprie Aug 1992
5147282 Kan Sep 1992
5163896 Suthanthiran et al. Nov 1992
5176617 Fischell et al. Jan 1993
5183455 Hayman et al. Feb 1993
5199939 Dake et al. Apr 1993
5213561 Weinstein et al. May 1993
5267960 Hayman et al. Dec 1993
5282781 Liprie Feb 1994
5302168 Hess Apr 1994
5322499 Liprie Jun 1994
5342283 Good Aug 1994
5344383 Liping Sep 1994
5354257 Roubin et al. Oct 1994
5370685 Stevens Dec 1994
5391139 Edmundson Feb 1995
5395300 Liprie Mar 1995
5405309 Carden, Jr. Apr 1995
5411466 Hess May 1995
5425720 Rogalsky et al. Jun 1995
5429582 William Jul 1995
5460592 Langton et al. Oct 1995
5484384 Fearnot Jan 1996
5498227 Mawad Mar 1996
5503613 Weinberger Apr 1996
5503614 Liprie Apr 1996
5532122 Drukier Jul 1996
5538494 Matsuda Jul 1996
5540659 Tierstein Jul 1996
5556389 Liprie Sep 1996
5575749 Liprie Nov 1996
5605530 Fischell et al. Feb 1997
5611767 Williams Mar 1997
5616114 Thornton et al. Apr 1997
5618266 Liprie Apr 1997
5624372 Liprie Apr 1997
5643171 Bradshaw et al. Jul 1997
5649924 Everett et al. Jul 1997
5653683 D'Andrea Aug 1997
5662580 Bradshaw et al. Sep 1997
5674177 Hehrlien et al. Oct 1997
5683345 Waksman et al. Nov 1997
5688220 Verin et al. Nov 1997
5707332 Weinberger Jan 1998
5713828 Coniglione Feb 1998
5720717 D'Andrea Feb 1998
5722984 Fischell et al. Mar 1998
5728042 Schwager Mar 1998
5730698 Fischell et al. Mar 1998
5782740 Schneiderman Jul 1998
5782742 Crocker et al. Jul 1998
5795286 Fischell et al. Aug 1998
5800333 Liprie Sep 1998
5803895 Kronholz et al. Sep 1998
5807231 Liprie Sep 1998
5816259 Rose Oct 1998
5816999 Bischoff et al. Oct 1998
5820553 Hughes Oct 1998
5906573 Aretz May 1999
5910101 Andrews et al. Jun 1999
5910102 Hastings Jun 1999
5913813 Williams et al. Jun 1999
5916143 Apple et al. Jun 1999
5919126 Armini Jul 1999
5924973 Weinberger Jul 1999
5924974 Loffler Jul 1999
5938582 Ciamacco, Jr. et al. Aug 1999
5947889 Hehrlein Sep 1999
5947924 Liprie Sep 1999
5947958 Woodard et al. Sep 1999
5957829 Thornton Sep 1999
5961439 Chernomorsky et al. Oct 1999
5967966 Kronholz et al. Oct 1999
5971909 Bradshaw et al. Oct 1999
5976106 Verin et al. Nov 1999
5997462 Loffler Dec 1999
5997463 Cutrer Dec 1999
6010445 Armini et al. Jan 2000
6013019 Fischell et al. Jan 2000
6013020 Meloul et al. Jan 2000
6024690 Lee et al. Feb 2000
6030333 Sioshansi et al. Feb 2000
6033357 Ciezki et al. Mar 2000
Foreign Referenced Citations (124)
Number Date Country
2166915 Aug 1996 CAX
0152124A3 Aug 1985 EPX
0158630A3 Oct 1985 EPX
0308630A1 Mar 1989 EPX
0 593 136 B1 Dec 1990 EPX
0433011A1 Jun 1991 EPX
0447745A2 Sep 1991 EPX
0466681A1 Jan 1992 EPX
0474994A1 Mar 1992 EPX
0 514 913 A2 May 1992 EPX
0 633 041 A1 Jul 1993 EPX
0 696 906 B1 Apr 1994 EPX
0 688 580 A1 Jun 1994 EPX
0621015A1 Oct 1994 EPX
0633041A1 Jan 1995 EPX
0668088A1 Aug 1995 EPX
0 778 051 A1 Dec 1995 EPX
0 686 342 Dec 1995 EPX
0686342A1 Dec 1995 EPX
0 754 473 A2 Jul 1996 EPX
0 754 472 A2 Jan 1997 EPX
0 801 961 A2 Apr 1997 EPX
0 813 894 A2 Dec 1997 EPX
0 810 004 Dec 1997 EPX
0 749 764 A1 Jun 1998 EPX
0 865 803 Sep 1998 EPX
0 904 798 Mar 1999 EPX
0 904 799 Mar 1999 EPX
3620123A1 Dec 1987 DEX
09102312 Aug 1992 DEX
19754870 Jan 1997 DEX
197 58 234 Jul 1999 DEX
198 07 727 Jul 1999 DEX
198 26 000 Dec 1999 DEX
198 25 999 Dec 1999 DEX
198 25 563 Dec 1999 DEX
198 29 447 Jan 2000 DEX
10-071210 Mar 1998 JPX
793158 Apr 1958 GBX
WO 8603124 Jun 1986 WOX
8903197 Apr 1989 WOX
9200776 Jan 1992 WOX
9203179 Mar 1992 WOX
9218051 Oct 1992 WOX
9304735 Mar 1993 WOX
WO 9304735 Mar 1993 WOX
9319804 Oct 1993 WOX
9319803 Oct 1993 WOX
9400847 Jan 1994 WOX
9416646 Aug 1994 WOX
WO 9425106 Nov 1994 WOX
WO 9426205 Nov 1994 WOX
WO 9507732 Mar 1995 WOX
9530384 Nov 1995 WOX
9606654 Mar 1996 WOX
WO 9610436 Apr 1996 WOX
WO 9614898 May 1996 WOX
WO 9613303 May 1996 WOX
9617654 Jun 1996 WOX
WO 9622121 Jul 1996 WOX
WO 9629943 Oct 1996 WOX
WO 9640352 Dec 1996 WOX
WO 9707740 Mar 1997 WOX
WO 9709937 Mar 1997 WOX
WO 9718012 May 1997 WOX
WO 9717029 May 1997 WOX
WO 9719706 Jun 1997 WOX
WO 9725102 Jul 1997 WOX
WO 9725103 Jul 1997 WOX
WO 9740889 Nov 1997 WOX
WO 9801183 Jan 1998 WOX
WO 9801184 Jan 1998 WOX
WO 9801185 Jan 1998 WOX
WO 9801186 Jan 1998 WOX
WO 9811936 Mar 1998 WOX
WO 9816151 Apr 1998 WOX
WO 9820935 May 1998 WOX
WO 9825674 Jun 1998 WOX
WO 9830273 Jul 1998 WOX
WO 9829049 Jul 1998 WOX
WO 9836769 Aug 1998 WOX
WO 9834681 Aug 1998 WOX
WO 9836788 Aug 1998 WOX
WO 9840032 Sep 1998 WOX
WO 9839063 Sep 1998 WOX
WO 9839062 Sep 1998 WOX
WO 9839052 Sep 1998 WOX
WO 9846309 Oct 1998 WOX
WO 9921615 May 1999 WOX
WO 9921616 May 1999 WOX
WO 9922774 May 1999 WOX
WO 9922775 May 1999 WOX
WO 9922812 May 1999 WOX
WO 9922815 May 1999 WOX
WO 9924116 May 1999 WOX
WO 9924117 May 1999 WOX
WO 9929354 Jun 1999 WOX
WO 9929370 Jun 1999 WOX
WO 9929371 Jun 1999 WOX
WO 9930779 Jun 1999 WOX
WO 9934969 Jul 1999 WOX
WO 9936121 Jul 1999 WOX
WO 9942162 Aug 1999 WOX
WO 9940974 Aug 1999 WOX
WO 9940973 Aug 1999 WOX
WO 9940972 Aug 1999 WOX
WO 9940971 Aug 1999 WOX
WO 9940970 Aug 1999 WOX
WO 9940962 Aug 1999 WOX
WO 9939628 Aug 1999 WOX
WO 9942163 Aug 1999 WOX
WO 9942177 Aug 1999 WOX
WO 9944686 Sep 1999 WOX
WO 9944687 Sep 1999 WOX
WO 9949935 Oct 1999 WOX
WO 9956825 Nov 1999 WOX
WO 9956828 Nov 1999 WOX
WO 99-61107 Dec 1999 WOX
WO 9962598 Dec 1999 WOX
WO 9966979 Dec 1999 WOX
WO 0003292 Jan 2000 WOX
WO 0004838 Feb 2000 WOX
WO 0004953 Feb 2000 WOX
WO 0009212 Feb 2000 WOX
Non-Patent Literature Citations (8)
Entry
Search Report in corresponding European patent application EP 95119124.6, together with Communication and one-page Annex.
"Strontium-90--Applikator fur interstitielle Bestrahlung der Hypophyse," Fortschritte auf dem Begiete der Rontgenstrahlen und den Nuklearmedizin, Holmer et al., pp. 574-578 (1967), with English translation.
Introduction to Modern Physics, Richtmyer, Kennard, and Lauritsen, Fifth Edition, 1955.
The Atomic Nucleus, Robley D. Evans, Ph.D., Massachusetts Institute of Technology, pp. 608-629, 1955.
"Strengthening mechanisms in Elgiloy", Journal of Materials Science 19 (1984), pp. 2815-2836.
Fort Wayne Metals Brochure--Drawn Filled Tubing.
Heat Treament, Structure and Properties of Nonferrous Alloys, Charlie R. Brooks, American Society for Metals, Jul. 1990, pp. 33, 51, and 330-331.
Mechanical Metallurgy, George R. Dieter, McGraw-Hill, Inc., 1976, p. 560.