[0001] The present invention relates to a crucible for a LUWPL, that is a Lucent waveguide
Plasma Light source.
[0002] In European Patent No
EP1307899, granted in our name there is claimed a light source comprising a waveguide configured
to be connected to an energy source and for receiving electromagnetic energy, and
a bulb coupled to the waveguide and containing a gas-fill that emits light when receiving
the electromagnetic energy from the waveguide, characterised in that:
- (a) the waveguide comprises a body consisting essentially of a dielectric material
having a dielectric constant greater than 2, a loss tangent less than 0.01, and a
DC breakdown threshold greater than 200 kilovolts/inch, 1inch being 2.54cm,
- (b) the wave guide is of a size and shape capable of supporting at least one electric
field maximum within the wave guide body at at least one operating frequency within
the range of 0.5 to 30GHz,
- (c) a cavity depends from a first side of the waveguide,
- (d) the bulb is positioned in the cavity at a location where there is an electric
field maximum during operation, the gas-fill forming a light emitting plasma when
receiving microwave energy from the resonating waveguide body, and
- (e) a microwave feed positioned within the waveguide body is adapted to receive microwave
energy from the energy source and is in intimate contact with the waveguide body.
[0003] In our
European Patent No 2,188,829 there is described and claimed a light source to be powered by microwave energy,
the source having:
- a body having a sealed void therein,
- a microwave-enclosing Faraday cage surrounding the body,
- the body within the Faraday cage being a resonant waveguide,
- a fill in the void of material excitable by microwave energy to form a light emitting
plasma therein, and
- an antenna arranged within the body for transmitting plasma-inducing, microwave energy
to the fill, the antenna having:
- a connection extending outside the body for coupling to a source of microwave energy;
wherein:
- the body is a solid plasma crucible of material which is lucent for exit of light
therefrom, and
- the Faraday cage is at least partially light transmitting for light exit from the
plasma crucible,
the arrangement being such that light from a plasma in the void can pass through the
plasma crucible and radiate from it via the cage.
[0004] We refer to this as our Light Emitting Resonator or LER patent. Its main claim as
immediately above is based, as regards its prior art portion, on the disclosure of
our
EP1307899, first above.
[0005] In our
European Patent Application No 08875663.0, published under No
WO2010055275, there is described and claimed a light source comprising:
- a lucent waveguide of solid dielectric material having:
- an at least partially light transmitting Faraday cage surrounding the waveguide, the
Faraday cage being adapted for light transmission radially,
- a bulb cavity within the waveguide and the Faraday cage and
- an antenna re-entrant within the waveguide and the Faraday cage and
- a bulb having a microwave excitable fill, the bulb being received in the bulb cavity.
[0006] We refer to this as our Clam Shell application, in that the lucent wave guide forms
a clam shell around the bulb.
[0007] As used in our LER patent, our Clam Shell application and this specification:
- "microwave" is not intended to refer to a precise frequency range. We use "microwave"
to mean the three order of magnitude range from around 300MHz to around 300GHz;
- "lucent" means that the material, of which an item described as lucent is comprised,
is transparent or translucent;
- "plasma crucible" means a closed body enclosing a plasma, the latter being in the
void [in the body] when the void's fill is excited by microwave energy from the antenna;
- "Faraday cage" means an electrically conductive enclosure of electromagnetic radiation,
which is at least substantially impermeable to electromagnetic waves at the operating,
i.e. microwave, frequencies.
[0008] The LER patent, the Clam Shell Application and certain LER improvement applications
have in common that they are in respect of:
A microwave plasma light source having:
- a Faraday cage:
- delimiting a waveguide and
- being at least partially lucent, and normally at least partially transparent, for
light emission from it, and
- normally having a non-lucent closure;
- a body of solid-dielectric, lucent material embodying the waveguide within the Faraday
cage;
- a closed void in the waveguide containing microwave excitable material; and
- provision for introducing plasma exciting microwaves into the waveguide;
the arrangement being such that on introduction of microwaves of a determined frequency
a plasma is established in the void and light is emitted via the Faraday cage.
[0010] A microwave plasma light source having:
- a fabrication of solid-dielectric, lucent material, having;
- a closed void containing electro-magnetic wave, normally microwave, excitable material;
and
- a Faraday cage:
- delimiting a waveguide,
- being at least partially lucent, and normally at least partially transparent, for
light emission from it,
- normally having a non-lucent closure and
- enclosing the fabrication;
- provision for introducing plasma exciting electro-magnetic waves, normally microwaves,
into the waveguide;
the arrangement being such that on introduction of electro-magnetic waves, normally
microwaves, of a determined frequency a plasma is established in the void and light
is emitted via the Faraday cage.
[0011] In the preferred embodiment of our LER patent, the void is formed directly in the
lucent waveguide, which is generally a quartz body. This exposes the quartz material
to high temperatures by radiation from the plasma and conduction from the gases surrounding
the plasma. It is because of this exposure that the term "solid plasma
crucible" is used in the LER patent, a crucible being a container for high temperature material.
This exposure can result in problems if the plasma causes micro-cracking of the material
of the crucible, which then propagate through it.
[0012] In our Clam Shell application, this problem is not so apparent in that a quartz bulb
having the void and excitable material is provided distinct from and inserted into
the lucent wave guide. The waveguide may be formed of two halves captivating the bulb
between them or a single body having a bore in which the bulb is received.
[0013] The object of the present invention is to provide an improved crucible for a LUWPL
of the LER type.
[0014] According to a first aspect of the invention there is provided a crucible for a LUWPL,
the crucible comprising:
- a waveguide body of lucent material having a bore;
- a tube of lucent material is provided in the bore, the tube:
- being closed at both ends,
- containing the excitable material in a void formed in its bore between its sealed
ends and
- being in intimate contact with the lucent material of the body.
[0015] According to a second aspect of the invention there is provided an intermediate product
in the manufacture of the crucible of the first aspect, the intermediate product comprising:
- a waveguide body of lucent material having a bore and
- a tube of lucent material provided in the bore in intimate contact with the lucent
material of the body.
[0016] Normally the waveguide body will be of fused quartz and the tube will be of drawn
fused quartz tube, free from micro-cracks inherent in the machining of the bore in
the body. Hereinbelow, the term "quartz" is used to indicate "fused quartz".
[0017] In use of the crucible of the invention, the bore is protected from the action of
the plasma gases and the intensity of heat inherent in bordering a plasma containing
void. Intimacy of contact in the bore between the tube and the body can be expected
to allow continuity of thermal and electrical properties throughout the crucible,
for instance in conduction of heat from the bore - albeit that quartz, the preferred
material, is a poor conductor of heat which is advantageous in allowing the void region
of the crucible to run hot.
[0018] Normally the lucent material of the tube will be the same or at least substantially
similar to that of the body. By substantially similar is intended that one or other
material may include additives such as to change its optical transmissivity and/or
its dielectric constant.
[0019] Whereas in metalworking arts, intimate contact can be achieved either by thermal
expansion/contraction of parts or by pressing of parts together, pressing is liable
to shatter quartz parts.
[0020] According to a third aspect of the invention there is provided a method in the manufacture
of the crucible of the first aspect including the steps of:
- providing a lucent waveguide body with a bore therein;
- inserting a lucent tube in the bore; and
- causing the tube to expand and/or the body to contract to bring the tube and the body
into intimate contact in the bore.
[0021] Whilst it is envisaged that the expansion/contraction could be achieved by heating
the body and/or cooling the tube prior to insertion of the tube in the bore, it is
preferably achieved with quartz tube by:
- heating the tube to its softening prior to insertion and
- inflating it on insertion.
[0022] Whilst it is envisaged that the heated tube could be inserted into a cool lucent
waveguide body, we prefer to preheat the body prior to the insertion, whereby the
tube does not tend to contract away from body on cooling after inflation.
[0023] Whilst the tube can be of plain uniform diameter; we prefer for it to have at least
a large diameter portion sized complementarily with the bore and a smaller diameter
portion for its sealing to enclosed the excitable material.
[0024] Whilst the distal/insert end of the tube can be unsealed on insertion, it is preferably
sealed prior to insertion. The bore can be a blind bore, with the sealed end of the
tube being inserted as far as the bottom of the bore, the bore is preferably a through
bore, with the distal end being inserted to extend to a determined extent.
[0025] Preferably, the insertion is as far as a stop on the side of the body opposite from
the insertion side. The stop could be a physical stop, which has the advantage of
supporting the sealed end of the tube against extension away from the body on inflation.
However an optical stop can be used alone or in addition to the physical stop. By
optical stop is meant that a light beam is interrupted by the sealed end when the
tube is correctly positioned, with the interruption causing an actuator advancing
the tube to stop the advance and cause the application of internal pressure in the
tube to inflate it. Alternatively other means of detecting that the sealed end of
the tube has reached its stop position can be envisaged.
[0026] Conveniently, the distal end is inserted through the bore to sufficient extent that
immediately beyond the opposite end orifices of the bore, the tube expands to a diameter
greater than the bore, outside it, where the tube is not constrained by the bore,
whereby the tube is physically restrained against axial movement with respect to the
body. For this the tube is heated along a length exceeding the length of the bore.
[0027] Alternatively, where the bore is a through bore, the distal end can be inserted to
be flush with the side of the body opposite from that at which the tube is inserted
into the body
[0028] Again, preferably the tube is heated whilst being monitored by a thermometer, such
as an infra-red detector, whereby the actuator can be caused to advance the tube as
soon as the tube has reached a temperature at which it is sufficiently soft to be
inflatable, yet still sufficiently rigid to be able to be inserted.
[0029] Closure of the proximal end of the tube can be conventional glass working techniques,
which can but need not involve upsetting and fusing of the material of the tube with
the material of the body. Further, the originally sealed end can be upset into more
intimate contact with its side of the body.
[0030] The non-sealed end is preferably sealed in two stages, (i.) remotely from the body
first after insertion of the excitable material and (ii.) close to the body thereafter,
with the intervening length of tube being removed.
[0031] Preferably, after the insertion of the excitable material and prior to the initial
sealing;
- the excitable material is caused to sublime and re-condense within the inflated portion
of the tube or in the tube in its extent from the body and
- volatile impurity introduced with excitable material is evacuated;
after initial sealing:
- excitable material condensed in the tube outside the body is caused to sublime and
re-condensed in the inflated tube inside the body or in the initially sealed end thereof
prior to final sealing.
[0032] To help understanding of the invention, a specific embodiment thereof will now be
described by way of example and with reference to the accompanying drawings, in which:
Figure 1 is a diagrammatic view of apparatus for manufacture of a lucent crucible
in accordance with the invention;
Figure 2 is a cross-sectional view of an intermediate product in the manufacture of
the crucible;
Figure 3 is a sectional perspective view of the manufactured crucible;
Figure 4 is a view similar to Figure 2 of a variant with a stepped tube prior to sealing;
and
Figure 5 is a cross-sectional view similar to Figure 4 of the varied lucent crucible
after sealing.
[0033] Referring to the drawings, a crucible 1 of the invention is formed from a wave guide
body 2 of fused quartz, typically it is 49mm in diameter and 20mm long for operation
in a Faraday cage closely enclosing it at a microwave resonance of 2.45GHz. It has
a central bore 3 of 6mm diameter through it, which is polished to optical clarity,
but not to the extent of reasonable certainty of removal of all micro-cracks resultant
from the process of boring. It also has an eccentric bore for receiving an antenna
for introducing microwaves.
[0034] Received within the central bore is a drawn quartz tube 4 of 1 mm nominal wall thickness,
i.e. 6mm nominal outside diameter, whose outer surface 5 has been brought into intimate
contact with the optically clear surface 6 of the bore, whereby crucible has for practical
purposes properties as if it were a single piece of quartz with the 4mm bore 7 at
the centre of the tube having the surface finish of a drawn tube. We postulate a test
of such intimacy of contact as follows, namely slicing the ends off the body say 3mm
from each end face 8, through the tube and the bores referred to. If the tube has
been brought into intimate contact, it can be expected to resist pressing from the
bore. (It should be noted that we propose alternative crucible structures with the
tube not in intimate contact in co-pending applications.)
[0035] The ends of the tube are sealed. One end 9 is largely as formed prior to insertion
of the tube 4 in the bore 2 and slightly inflated on insertion. The other end 10 has
a closure formed, by glass blowing techniques, after the bore was inserted. Inside
the sealed tube is a charge of material excitable by microwave energy to form a light
emitting plasma on the axis of the tube.
[0036] Manufacture of the crucible is performed with equipment including:
- a support 11 for a lucent body 2, the body having been bored, possibly polished and
pre-heated close to softening temperature but yet not so close as to cause it to lose
its shape in movement from a pre-heating oven (not shown) to the support;
- a chuck 12 for holding the tube 4, already sealed at its end 9 without any part of
the end having a diameter greater than that of the rest of the tube, concentric with
the bore 3;
- a radiant heater 14 for the extent 15 of the tube, equal to the thickness of the body
1 plus a margin, to be received in the body;
- a thermometer 16 for monitoring the temperature to which the tube is heated;
- means 17 for optically detecting insertion of the tube through the body to a determined
protrusion 18,
- means 19 for admitting inflation gas to the interior of the tube, the inflation means
including:
- a pressurised gas source 20,
- an admission valve 21,
- a flexible connection 22 allowing advance of the chuck and the tube 4 during its insertion
and
- a rotary connection 23 allowing rotation of the tube 4 during its heating;
- means 24 for advancing the chuck and the tube with it;
- a controller 25.
[0037] Operation of this equipment under the control of the controller 25 is as follows:
- a) the body 2 is preheated and placed on the support, with its bore concentric with
the tube 4 supported in the chuck and connected to the inflation means;
- b) the tube is heated with the chuck being rotated for evenness of heating;
- c) when the temperature of the tube is detected to be the softening point of the quartz
of the tube, its rotation is stopped and it is advanced into the bore 3 in the body
2;
- d) advance is stopped when the distal, sealed end is detected to have reached the
determined protrusion 18;
- e) simultaneously with the advance being stopped, inflation gas is admitted into the
tube, to inflate it albeit marginally, and bring the outer surface 5 of the tube into
intimate contact with the surface 6 of the bore 4, the inflation also expanding the
tube immediately outside the bore, to further assure the fixture of the tube in the
bore;
- f) the intermediate product so formed is set aside to cool, or allowed to cool partially
or indeed, it can be processed further whilst still hot.
[0038] The further processing steps are:
g) disconnection of the inflation gas source and connection to a vacuum pump (not
shown);
h) evacuation of the tube;
i) insertion of a pellet of excitable material - with the precaution that the intermediate
crucible product is not too hot to volatilise the excitable material;
j) admission of the inert gas into the evacuated tube;
k) heating of the tube remote from the body and working of the tube to seal it;
1) heating of the tube close to the body and working it to form a second and final
seal close to the body with the seal upset to extend to a greater diameter than the
original tube diameter. The intermediate length of the tube between the first and
second seals is removed.
[0039] The invention is not intended to be restricted to the details of the above described
embodiment. Particularly when the tube is arranged to be inserted down vertically
into the lucent body, the chuck may not be rotated, where the heater can be relied
upon not to distort the tube in bending. Indeed if such arrangement is used the chuck
can be replaced with a simpler clamp.
[0040] Further, it is likely that the pellet of excitable material will contain volatile
impurities in particular hydrogen iodide, whilst the excitable material itself is
solid at room temperature and volatile at higher temperatures than that of the volatile
impurities. For removal of the impurities, the pellet is introduced - as in step (i.)
above - when the intermediate crucible product is still above the impurity volatilisation
temperature. Alternatively, if the temperature has dropped, heat is applied to the
closed end 9 of the tube and the impurity is volatised and evacuated via the tube
which is evacuated. If the intermediate product is cool enough the sublimed pellet
material will condense in the inflated portion of the tube within the lucent body
2. Alternatively the tube extending from the body can be cooled by applied air flow
adjacent the body for re-condensing there. Then the inert gas is introduced as per
step (j.) and the remote end of the tube is sealed as in step (k.). The closed end
and/or the inflated portion, with the body 2, is cooled. Prior to sealing as in step
(1.), at least where the excitable material has condensed in the tube, the latter
is heated to re-sublime the material which then re-condenses on the closed end 9 or
the inflated portion of the tube within the body. The sealing step (1.) can then be
completed as above with the excitable material captivated.
[0041] The radiant heater can be an ohmic heater or a gas torch or indeed an inductively
heated carbon block.
[0042] The optical detection means can be an LED on a photodiode. Alternatively a camera
with suitable image recognition software can be used. Again, the detection means can
be augmented with a physical stop.
[0043] We would normally expect the best optical performance of the light source if the
excitable-material / plasma void extends to the full thickness of the body, which
involves the stop being spaced from the end face from which the sealed end of the
tube extends. Nevertheless, we can envisage that it may be advantageous to provide
the stop at the this end face, so that the inflation of the tube is wholly within
the bore in the body.
[0044] Whilst we believe that best results are likely to be achieved if the surface 6 of
the bore is polished to optical clarity; it may be possible to prepare it to a lesser
extent, for instance by fine grinding.
[0045] As regards the wall thickness of the tube is concerned, we would emphasise that the
dimension given of 1mm is merely exemplary. We expect 1.5mm and 2mm and indeed other
wall thickness quartz tubes to be inflatable and indeed tubes of other diameters from
the 6mm example to be inflatable. Further, whilst nominal 6mm bore 3 and 6mm outside
diameter tube are referred to above, for normal engineering fit reasons, the 0.5mm
clearance prior to inflation will normally be required, typically by boring 0.5mm
oversize and expanding the tube through this clearance. To achieve a 4mm bore, the
initial bore before inflation is smaller than 4mm.
[0046] Furthermore, we do not need for the inflated tube to extend beyond the end of the
body opposite from the insertion side, and the initially sealed end can be inserted
to be flush with side of the body opposite from the insertion side. Such a variant
is shown in Figures 4 & 5. A quartz body 102 has a central bore 103. A quartz tube
104 worked to capsule form has a large diameter parallel, end portion 1041 with an
outside diameter complementary to the bore 103. It is worked to have a flat end 1042,
which is flush with one side 1021 of the body in the finished product. It is also
worked to have an intermediate diameter portion 1043 and a small diameter portion
1044. It can be formed from two or more pieces fused together. The shoulder 1045 between
the large diameter and the intermediate diameter portions 1041,1043 is spaced from
the flat end by a distance equal to the thickness of the body. Thus on insertion of
the heated large diameter portion in the bore 103 and its inflation with its end 1042
flush with the side 1021, the shoulder falls flush with the other surface 1022 of
the body. After insertion of the excitable material, driving off of the impurities,
and preliminary sealing, the final seal is made at the intermediate portion, leaving
a sealed tip proud of the surface 1022.
1. A crucible (1) for a Lucent Waveguide Plasma Light source, LUWPL, the crucible comprising:
• a waveguide body (2) of lucent material having a body (3);
• a tube (4) of lucent material is provided in the bore, the tube:
• being closed at both ends,
• containing an excitable material in a void formed in its bore between its sealed
ends and
• being in intimate contact with the lucent material of the body.
2. A crucible for a LUWPL as claimed in claim 1, wherein the lucent material of the tube
will be the same to that of the body.
3. A crucible for a LUWPL as claimed in claim 1 or claim 2, wherein the waveguide body
and the tube are of fused quartz, the quartz tube preferably being a drawn quartz
tube.
4. An intermediate product in the manufacture of the crucible of any one of claims 1
to 3, the intermediate product comprising:
• a waveguide body of lucent material having a bore and
• a tube of lucent material provided in the bore in intimate contact with the lucent
material of the body.
5. A method in the manufacture of the crucible of any one of claims 1 to 3, including
the steps of:
• providing a lucent waveguide body with a bore therein;
• inserting a lucent tube in the bore; and
• causing the tube to expand and/or the body to contract to bring the tube and the
body into intimate contact in the bore.
6. A method as claimed in claim 5, wherein:
• the expansion/contraction is effected by heating the body and/or cooling the tube
prior to insertion of the tube in the bore, and
• the expansion/contraction is preferably effected with quartz tube by: heating the
tube to its softening point prior to insertion and inflating it on insertion.
7. A method as claimed in claim 6, wherein:
• the heated tube is inserted into a cool lucent waveguide body; or
• the body is preheated prior to the insertion of the heated tube; or the tube is
heated whilst being monitored by a thermometer, such as an infra-red detector,
whereby an actuator is caused to advance the tube as soon as the tube has
reached a temperature at which it is sufficiently soft to be inflatable, yet still
sufficiently rigid to be able to be inserted.
8. A method as claimed in either of claims 6 and 7, wherein the distal/insert end of
the tube is:
• unsealed on insertion, or
• sealed prior to insertion
9. A method as claimed in claim 8, wherein the bore is:
• a blind bore and the sealed end of the tube is inserted as far as the bottom of
the bore, or
• a through bore and the distal end is inserted to extend to a determined extent from
the side of the body opposite from that at which the tube is inserted into the body.
10. A method as claimed in claim 9, wherein the distal end is inserted through the bore
to sufficient extent that, immediately beyond opposite end orifices of the bore outside
it, the tube expands to a diameter greater than the bore, where the tube is not constrained
by the bore, whereby the tube is physically restrained against axial movement with
respect to the body, the tube having been heated along a length exceeding the length
of the bore.
11. A method as claimed in claim 8, wherein the bore is a through bore and the distal
end is:
• inserted to be flush with the side of the body opposite from that at which the tube
is inserted into the body, or
• inserted as far as a stop on the side of the body opposite from the insertion side.
12. A method as claimed in claim 11, wherein the stop is a physical stop, or the stop
is an optical stop used alone or in addition to a physical stop, a light beam being
provided and interrupted by the sealed end when the tube is correctly positioned,
with the interruption causing an actuator advancing the tube to stop the advance and
cause the application of internal pressure in the tube to inflate it.
13. A method as claimed in any one of claims 5 to 12, wherein the tube is:
• of plain uniform diameter, or
• stepped having at least a large diameter portion sized complementarily with the
bore and a smaller diameter portion for its sealing to enclose the excitable material.
14. A method as claimed in claim 13, wherein sealing of the proximal end of the tube is
effected by glass working techniques, preferably including upsetting and fusing of
the material of the tube with the material of the body and upsetting of the sealed
distal end into more intimate contact with its side of the body.
15. A method as claimed in anyone of claims 9 to 14, wherein the proximal end of the tube
is sealed in two stages, (i.) remotely from the body first after insertion of the
excitable material and (ii.) close to the body thereafter, with the intervening length
of tube being removed.
16. A method as claimed in claim 13, wherein after the insertion of the excitable material
and prior to the initial sealing:
• the excitable material is caused to sublime and re-condense within the inflated
portion of the tube or in the tube in its extent from the body and
• volatile impurity introduced with excitable material is evacuated;
after initial sealing:
• excitable material condensed in the tube outside the body is caused to sublime and
re-condensed in the inflated tube inside the body or in the initially sealed end thereof
prior to final sealing.
1. Tiegel (1) für eine lichtdurchlässige Wellenleiter Plasma-Lichtquelle, LUWPL, wobei
der Tiegel aufweist:
• einen Wellenleiter-Körper (3) aus lichtdurchlässigem Material mit einer Bohrung
(3);
• ein in der Bohrung angeordnetes Rohr (4) aus lichtdurchlässigem Material, wobei
das Rohr:
• an beiden Enden geschlossen ist,
• in dem Hohlraum seiner Bohrung zwischen den verschlossenen Enden ein erregbares
Material enthält, und
• in einem innigen Kontakt mit dem lichtdurchlässigen Material des Körpers steht.
2. Tiegel für eine LUWPL nach Anspruch 1, dadurch gekennzeichnet, dass das lichtdurchlässige Material des Rohres dasselbe wie das des Körpers ist.
3. Tiegel für eine LUWPL nach Anspruch 1 oder Anspruch 2, dadurch gekennzeichnet, dass der Wellenleiter-Körper und das Rohr aus Quarzglas bestehen, wobei das Quarzrohr
vorzugsweise ein gezogenes Quarzrohr ist.
4. Zwischenprodukt bei der Herstellung des Tiegels nach einem der Ansprüche 1 bis 3,
wobei das Zwischenprodukt aufweist:
• einen Wellenleiter-Körper aus lichtdurchlässigem Material mit einer Bohrung, und
• ein Rohr aus lichtdurchlässigem Material, das in der Bohrung in innigem Kontakt
mit dem lichtdurchlässigen Material des Körpers angeordnet ist.
5. Verfahren zur Herstellung des Tiegels nach einem der Ansprüche 1 bis 3, enthaltend
die Verfahrensschritte:
• Bereitstellen eines lichtdurchlässigen Wellenleiter-Körpers mit einer darin angeordneten
Bohrung;
• Einführen eines lichtdurchlässigen Rohrs in die Bohrung; und
• Bewirken, dass das Rohr expandiert und/oder sich der Körper zusammenzieht, um das
Rohr und den Körper in der Bohrung in innigen Kontakt miteinander zu bringen.
6. Verfahren nach Anspruch 5,
dadurch gekennzeichnet, dass:
• die Expansion/Kontraktion erfolgt durch Erwärmen des Körpers und/oder Abkühlen des
Rohrs vor dessen Einführung in der Bohrung, und
• die Expansion/Kontraktion bei Verwendung eines Quarzrohrs vorzugsweise erfolgt durch:
Erwärmen des Rohrs bis zu seiner Erweichungstemperatur vor der Einführung und Aufblähen
des Rohres beim Einführvorgang.
7. Verfahren nach Anspruch 6,
dadurch gekennzeichnet, dass:
• das erwärmte Rohr in einen kühlen, lichtdurchlässigen Wellenleiter-Körper eingeführt
wird; oder
• der Körper vor der Einführung des erwärmten Rohrs vorgewärmt wird; oder
• das Rohr unter Überwachung mit einem Thermometer, wie beispielsweise einem Infrarot-Detektor,
erwärmt wird, wodurch ein Aktuator veranlasst wird, das Rohr vorzuschieben, sobald
es eine Temperatur erreicht hat, bei der es ausreichend weich ist, um aufgebläht werden
zu können, jedoch noch immer ausreichend steif ist, um eingeführt werden zu können.
8. Verfahren nach einem der Ansprüche 6 oder 7,
dadurch gekennzeichnet, dass das distale/Einführ-Ende des Rohres:
• beim Einführen unverschlossen ist, oder
• vor der Einführen verschlossen wurde.
9. Verfahren nach Anspruch 8,
dadurch gekennzeichnet, dass die Bohrung:
• eine Sacklochbohrung ist und das geschlossene Ende des Rohres bis zum Grund der
Bohrung eingeführt wird, oder
• eine durchgehende Bohrung ist und das distale Ende soweit eingeführt wird, dass
es sich bis zu einem vorbestimmten Maß an der Seite des Körpers erstreckt, die sich
gegenüber der Seite befindet, an der das Rohr in den Körper eingeführt wird.
10. Verfahren nach Anspruch 9, dadurch gekennzeichnet, dass das distale Ende durch die Bohrung soweit eingeführt wird, dass sich das Rohr unmittelbar
hinter den gegenüberliegenden Endöffnungen der Bohrung außerhalb dieser auf einen
Durchmesser aufweitet, der größer ist als der der Bohrung, wo das Rohr nicht durch
die Bohrung begrenzt ist, wodurch das Rohr gegen eine axiale Bewegung relativ zu dem
Körper physikalisch zurückgehalten wird , wobei das Rohr auf einer Länge erhitzt wurde,
die die Länge der Bohrung übersteigt.
11. Verfahren nach Anspruch 8,
dadurch gekennzeichnet, dass die Bohrung eine Durchgangsbohrung ist und das distale Ende:
• so eingeführt wird, dass es bündig mit der Seite des Körpers ist, die gegenüber
der Seite liegt, von der das Rohr in den Körper eingeführt wird, oder
• bis zu einem Anschlag an der Seite des Körpers eingeführt wird, die gegenüber der
Einführseite liegt.
12. Verfahren nach Anspruch 11, dadurch gekennzeichnet, dass der Anschlag ein körperlicher Anschlag ist oder ein optischer Anschlag ist, der für
sich genommen oder in Verbindung mit einem körperlichen Anschlag verwendet wird, wobei
ein Lichtstrahls vorgesehen ist, der von dem geschlossenen Ende unterbrochen wird,
wenn das Rohr richtig positioniert ist, wobei die Unterbrechung bewirkt, dass ein
das Rohr vorschiebender Antrieb den Vorschub stoppt und eine Beaufschlagung des Innendrucks
in dem Rohr bewirkt, um es aufzublähen.
13. Verfahren nach einem der Ansprüche 5 bis 12, behauptet,
dadurch gekennzeichnet, dass das Rohr:
• einen einfachen, einheitlichen Durchmesser aufweist, oder
• gestuft ausgebildet ist, mit mindestens einen Abschnitt großen Durchmessers, der
komplementär zu der Bohrung bemessen ist, und einem Bereich kleineren Durchmessers
zum Abdichten, um das erregbare Material einschließen.
14. Verfahren nach Anspruch 13, dadurch gekennzeichnet, dass die Abdichtung des proximalen Endes des Rohres durch Glasbearbeitstechniken bewirkt
wird, vorzugsweise einschließlich Stauchen und Aufschmelzen des Materials des Rohres
mit dem Material des Körpers und Stauchen des versiegelten distalen Endes in innigeren
Kontakt mit seiner Seite des Körpers.
15. Verfahren nach einem der Ansprüche 9 bis 14, dadurch gekennzeichnet, dass das proximale Ende des Rohres in zwei Stufen versiegelt wird, (i.) zunächst im Abstand
von dem Körper nach dem Einbringen des erregbaren Materials, und (ii.) anschließend
nahe dem Körper, wobei der dazwischen liegende Abschnitt des Rohrs entfernt wird.
16. Verfahren nach Anspruch 13,
dadurch gekennzeichnet, dass nach dem Einbringen des erregbaren Materials und vor der ersten Versiegelung:
• das erregbare Material veranlasst wird, zu sublimieren und im Inneren des aufgeblähten
Abschnitts des Rohrs oder dem Rohr in dessen Vorstand vom Körper wieder zu kondensieren
• flüchtige Verunreinigungen, die mit dem erregbaren Material eingebracht wurden,
evakuiert werden;
nach der ersten Versiegelung:
• erregbares Material, das in dem Rohr außerhalb des Körpers kondensiert ist, veranlasst
wird, zu sublimieren und in dem aufgeblähten Rohr im Inneren des Körpers oder in dessen
vorläufig verschlossenen Endbereich wieder zu kondensieren, bevor die endgültige Versiegelung
erfolgt.
1. Un creuset (1) pour une source lumineuse à plasma à guide d'ondes transparent ou translucide,
LUWPL, le creuset comprenant :
· un corps de guide d'ondes (2) en matériau transparent ou translucide possédant un
trou (3) ;
· un tube (4) de matériau transparent ou translucide qui est disposé dans le trou,
le tube :
· étant fermé aux deux extrémités,
· contenant un matériau excitable dans un vide formé dans son trou entre ses extrémités
obturées, et
· étant en contact intime avec le matériau transparent ou translucide du corps.
2. Un creuset pour une LUWPL selon la revendication 1, dans lequel le matériau transparent
ou translucide du tube sera le même que celui du corps.
3. Un creuset pour une LUWPL selon la revendication 1 ou la revendication 2, dans lequel
le corps de guide d'ondes et le tube sont en quartz fondu, le tube en quartz étant
de préférence un tube en quartz étiré.
4. Un produit intermédiaire de la fabrication du creuset de l'une quelconque des revendications
1 à 3, le produit intermédiaire comprenant :
· un corps de guide d'ondes de matériau transparent ou translucide possédant un trou,
et
· un tube de matériau transparent ou translucide disposé dans le trou en contact intime
avec le matériau transparent ou translucide du corps.
5. Un procédé de fabrication du creuset de l'une quelconque des revendications 1 à 3,
comprenant les étapes suivantes :
· obtenir un corps de guide d'ondes transparent ou translucide avec un trou dedans
;
· insérer un tube transparent ou translucide dans le trou ; et
· provoquer la dilatation du tube et/ou rétracter le corps pour amener le tube et
le corps en contact intime dans le trou.
6. Un procédé selon la revendication 5, dans lequel :
· la dilatation/rétraction est réalisée par chauffage du corps et/ou refroidissement
du tube avant l'insertion du tube dans le trou ; et
· la dilatation/rétraction est de préférence réalisée avec un tube de quartz par :
chauffage du tube jusqu'à son point de ramollissement avant insertion et gonflement
de celui-ci à l'insertion.
7. Un procédé selon la revendication 6, dans lequel :
· le tube chauffé est inséré dans un corps de guide d'ondes transparent ou translucide
froid ; ou
· le corps est préchauffé avant l'insertion du tube chauffé ; ou
· le tube est chauffé tout en étant surveillé par un thermomètre, tel qu'un détecteur
infrarouge,
de manière à faire en sorte qu'un actionneur puisse faire avancer le tube dès que
le tube a atteint une température à laquelle il est suffisamment ramolli pour être
gonflable, tout en étant suffisamment rigide pour pouvoir être inséré.
8. Un procédé selon l'une des revendications 6 et 7, dans lequel l'extrémité distale/d'insertion
du tube est :
· obturée à l'insertion, ou
· obturée avant l'insertion.
9. Un procédé selon la revendication 8, dans lequel le trou est :
· un trou borgne et l'extrémité obturée du tube est insérée jusqu'au fond du trou,
ou
· un trou traversant et l'extrémité distale est insérée pour s'étendre sur une étendue
déterminée à partir du côté du corps opposé de celui où le tube est inséré dans le
corps.
10. Un procédé selon la revendication 9, dans lequel l'extrémité distale est insérée au
travers du trou pour s'étendre de façon suffisante pour que, immédiatement au-delà
d'orifices d'extrémités opposées du trou en dehors de celui-ci, le tube se dilate
jusqu'à un diamètre supérieur à celui du trou, le tube n'étant pas contraint par le
trou, de sorte que le tube soit physiquement empêché de se déplacer axialement par
rapport au corps, le tube ayant été chauffé sur une longueur dépassant la longueur
du trou.
11. Un procédé selon la revendication 8, dans lequel le trou est un trou traversant et
l'extrémité distale est :
· insérée pour arriver au ras du côté du corps opposé de celui où le tube est inséré
dans le corps, ou
· insérée jusqu'à une butée du côté du corps opposé au côté de l'insertion.
12. Un procédé selon la revendication 11, dans lequel la butée est une butée physique,
ou la butée est une butée optique utilisée seule ou en supplément d'une butée physique,
un faisceau lumineux étant produit et interrompu par l'extrémité obturée lorsque le
tube est correctement positionné, l'interruption provoquant l'arrêt de l'avance par
un actionneur faisant avancer le tube et faisant en sorte qu'une pression interne
soit appliquée dans le tube pour le gonfler.
13. Un procédé selon l'une des revendications 5 à 12, dans lequel le tube est :
· de diamètre uniforme régulier, ou
· étagé avec au moins une partie de plus grand diamètre dimensionnée de façon complémentaire
par rapport au trou et une partie de plus faible diamètre pour son obturation afin
d'enfermer le matériau excitable.
14. Un procédé selon la revendication 13, dans lequel l'obturation de l'extrémité proximale
du tube est réalisée par des techniques de verrerie, de préférence incluant un refoulement
et une fusion du matériau du tube avec le matériau du corps et un refoulement de l'extrémité
distale obturée en contact plus intime avec son côté du corps.
15. Un procédé selon l'une des revendications 9 à 14, dans lequel l'extrémité proximale
du tube est obturée en deux étapes, (i.) tout d'abord à distance du corps après insertion
du matériau excitable et (ii.) ensuite à proximité du corps, avec élimination de la
longueur intercalaire du tube.
16. Un procédé selon la revendication 13, dans lequel après l'insertion du matériau excitable
et avant l'obturation initiale :
· on fait en sorte que le matériau excitable se sublime et se recondense à l'intérieur
de la partie gonflée du tube ou dans le tube dans son prolongement depuis le corps,
et
· on évacue les impuretés volatiles introduites avec le matériau excitable ;
après l'obturation initiale :
· on fait en sorte que le matériau excitable condensé dans le tube à l'extérieur du
corps se sublime et se recondense dans le tube gonflé à l'intérieur du corps ou dans
l'extrémité initialement obturée de celui-ci avant l'obturation finale.