throbber
IPR2014-01073
`U.S. Patent No. 6,896,773
`
`
`
`UNITED STATES PATENT AND TRADEMARK OFFICE
`__________________
`
`BEFORE THE PATENT TRIAL AND APPEAL BOARD
`__________________
`
`
`
`ADVANCED MICRO DEVICES, INC., RENESAS ELECTRONICS
`CORPORATION, RENESAS ELECTRONICS AMERICA, INC.,
`GLOBAL FOUNDRIES U.S., INC., GLOBALFOUNDRIES DRESDEN
`MODULE ONE LLC & CO. KG, GLOBALFOUNDRIES DRESDEN
`MODULE TWO LLC & CO. KG, TOSHIBA AMERICA ELECTRONIC
`COMPONENTS, INC., TOSHIBA AMERICA INC., TOSHIBA
`AMERICA INFORMATION SYSTEMS,
`
`Petitioners
`
`v.
`
`ZOND, LLC
`Patent Owner
`__________________
`
`Case IPR2014-008291
`Patent 6,805,779
`__________________
`
`
`
`ZOND LLC’S PATENT OWNER RESPONSE
`
`
`1 Cases IPR2014-00859 and IPR2014-01072 have been joined with the instant
`
`proceeding.
`
`

`
`IPR2014-01073
`U.S. Patent No. 6,896,773
`
`
`
`TABLE OF CONTENTS
`
`I. INTRODUCTION .......................................................................................................................1
`
`II. TECHNOLOGY BACKGROUND ...........................................................................................7
`
`A.
`
`B.
`
`Overview Of Plasma Generation ...................................................................................7
`
`The ’779 patent: Dr. Chistyakov invents a new plasma generator containing a
`feed gas source, an excited atom source with a magnet that traps electrons, a
`plasma chamber that confines excited atoms, and an energy source that ionizes
`the confined excited atoms in a multi-step ionization process. .....................................9
`
`C.
`
`The Petitioners Mischaracterized The File History. ....................................................13
`
`III. SUMMARY OF THE INSTITUTED GROUNDS FOR REVIEW .......................................14
`
`IV. CLAIM CONSTRUCTION. ..................................................................................................14
`
`A.
`
`The construction of “metastable atoms,” “multi step ionization,” and “excited
`atoms.” .........................................................................................................................15
`
`B.
`
`The construction of the means plus function limitations .............................................16
`
`V. THE PETITIONERS CANNOT PREVAIL ON ANY CHALLENGED CLAIM OF
`THE ’779 PATENT. ...............................................................................................................18
`
`A.
`
`The Petition failed to demonstrate that a skilled artisan would have been
`motivated to combine the teachings of the prior art references to achieve the
`claimed invention of the ’779 patent with a reasonable expectation of success
`or that combining the teachings of the prior art would have led to predictable
`results. ..........................................................................................................................19
`
`1.
`
`Scope and content of prior art. ...............................................................................21
`
`a.
`
`b.
`
`Iwamura ...........................................................................................................22
`
`Pinsley and Angelbeck .....................................................................................23
`
`2.
`
`The Petitioner Failed To Show That It Would Have Been Obvious To
`Combine The Laser Of Angelbeck Or Pinsley With The Plasma Treatment
`Apparatus Of Iwamura With A Reasonable Expectation Of Success. ..................24
`
`B.
`
`The Petition failed to demonstrate how the alleged combinations teach every
`element of the challenged claims. ................................................................................27
`
`
`
`ii
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`

`
`1.
`
`2.
`
`3.
`
`4.
`
`5.
`
`6.
`
`7.
`
`8.
`
`9.
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`IPR2014-01073
`U.S. Patent No. 6,896,773
`
`The combination of Iwamura and Angelbeck Does Not Teach “an excited
`atom source that receives ground state atoms from the feed from the
`ground state atoms,” As Recited In Claim 1 And As gas source … the
`excited atom source generating excited atoms Similarly Recited In
`Independent Claim 18. ...........................................................................................28
`
`The combination of Iwamura, Angelbeck and Pinsley does not teach “the
`excited atom source comprising a magnet that generates a magnetic field
`for substantially trapping electrons proximate to the ground state atoms”
`as recited in independent claim 1 and as similarly recited in independent
`claim 18. .................................................................................................................31
`
`The combination of Iwamura, Angelbeck and Pinsley does not teach “a
`plasma chamber that is coupled to the excited atom source,” as recited in
`independent claim 1 and as similarly recited in independent claim 18. ................36
`
`The combination of Iwamura, Angelbeck and Pinsley does not teach “the
`plasma chamber confining a volume of excited atoms generated by the
`excited atom source” as recited in independent claim 1 and as similarly
`recited in independent claim 18. ............................................................................38
`
`The combination of Iwamura, Angelbeck and Pinsley does not teach “an
`energy source that is coupled to the volume of excited atoms confined by
`the plasma chamber” as recited in independent claim 1 and as similarly
`recited in independent claim 18. ............................................................................39
`
`The combination of Iwamura, Angelbeck, and Pinsley does not teach “the
`energy source raising an energy of excited atoms in the volume of excited
`atoms so that at least a portion of the excited atoms in the volume of
`excited atoms is ionized,” as recited in independent claim 1 and as
`similarly recited in independent claim 18. .............................................................40
`
`The Combination of Iwamura, Angelbeck, and Pinsley Does Not
`Teach “an electron/ion absorber that receives the excited atoms from
`the excited atom source, the electron/ion absorber trapping electrons
`and ions,” as recited in dependent claim 16, and as simlarly recited in
`dependent claims 28 and 42. ...............................................................................41
`
`The combination of Iwamura, Angelbeck and Pinsley Does Not Teach
`“means for generating a volume of metastable atoms from the volume
`of ground state atoms,” As Recited In Independent Claim 41, And As
`Similarly Recited in Claim 46 .............................................................................43
`
`The combination of Iwamura, Angelbeck and Pinsley does not teach
`“means for generating a magnetic field proximate to a volume of
`ground state atoms to substantially trap electrons proximate to the
`
`
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`iii
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`

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`IPR2014-01073
`U.S. Patent No. 6,896,773
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`10.
`
`11.
`
`12.
`
`13.
`
`14.
`
`15.
`
`volume of ground state atoms,” as recited in independent claim 41 and
`as similarly recited in independent claim 46. .....................................................47
`
`The combination of Iwamura, Angelbeck, and Pinsley does not teach
`“means for raising an energy of the metastable atoms so that at least a
`portion of the volume of metastable atoms is ionized,” as recited in
`independent claim 41 and as similarly recited in independent claim 46. ........50
`
`The combination of Iwamura, Angelbeck and Pinsley Does Not Teach
`“an excited atom source that is coupled to the feed gas source, the
`excited atom source generating excited atoms from the ground state
`atoms,” As Recited In Independent Claim 45 ...................................................52
`
`The combination of Iwamura, Angelbeck and Pinsley does not teach
`“an electron/ion absorber that receives the excited atoms generated by
`the excited atom source and then traps electrons and ions,” as recited
`in independent claim 45. ......................................................................................53
`
`The combination of Iwamura, Angelbeck and Pinsley does not teach
`“a plasma chamber that is coupled to the electron/ion absorber, the
`plasma chamber confining a volume of excited atoms generated by the
`excited atom source,” as recited in independent claim 45. ...............................55
`
`The combination of Iwamura, Angelbeck and Pinsley does not teach
`“an energy source that is coupled to the volume of excited atoms
`confined by the plasma chamber,” as recited in independent claim 45. ..........56
`
`The combination of Iwamura, Angelbeck, and Pinsley does not teach
`“the energy source raising an energy of excited atoms in the volume of
`excited atoms so that at least a portion of the excited atoms in the
`volume of excited atoms is ionized,” as recited in independent claim
`45. ..........................................................................................................................57
`
`C.
`
`Petitioner Failed To Demonstrate That Claim 46 Is Anticipated By Iwamura............59
`
`VI. CONCLUSION.......................................................................................................................60
`
`
`
`iv
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`

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`IPR2014-01073
`U.S. Patent No. 6,896,773
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`Exhibit List
`
`Description
`
`Exhibit
`No.
`Ex. 2004 Transcript of deposition of Dr. Kortshagen, Petitioners’ expert, for
`the ’779 Patent, 1/16/2015.
`
`Ex. 2005 Declaration of Dr. Hartsough, Patent Owner’s expert.
`
`
`
`v
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`

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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`I. INTRODUCTION
`
`The Petitioners’ arguments hinge on fanciful misreadings of the prior art
`
`by their proffered expert, Dr. Kortshagen. As will be shown below, neither
`
`Iwamura, Angelbeck nor Pinsley teaches a “metastable atom source
`
`comprising a magnet that generates a magnetic field for substantially trapping
`
`electrons proximate to the ground state atoms,” as recited in claim 18. Once
`
`the Board recognizes that Dr. Kortshagen essentially invented some of the
`
`alleged “teachings” in Iwamura, Angelbeck, or Pinsley to suit the Petitioners’
`
`objectives, the Board should agree to confirm the challenged claims.
`
`The ’779 patent discloses and illustrates in FIG. 6 (reproduced on the
`
`next page below) a metastable atom source 500 including a chamber 502, first
`
`504a, b and second magnets 506a, b that create magnetic fields 508a, b through
`
`the chamber 502. A power supply 510 is coupled to the metastable atom
`
`source 500. A gas line 528 is coupled to an input 530 of the chamber 502. An
`
`output 532 of the chamber 502 is coupled to an input 534 of an electron/ion
`
`absorber 536. In operation, ground state atoms 208 from the gas source (not
`
`shown) flow to the metastable atom source 500 through the input 530 of the
`
`chamber 502. The ground state atoms 208 flow between the first electrode 524
`
`and the second electrode 526. The first 524 and the second electrodes 526 are
`
`energized by the power supply 510, such that an electric field is created that
`
`
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`1
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`

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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`generates a discharge in a discharge region 544 between the first 524 and the
`
`second electrodes 526. The ground state atoms 208 that are injected through
`
`the discharge region 540 are energized to a metastable state.
`
`
`
`
`
`In one embodiment, ions in the chamber 502 impact the more negatively
`
`biased electrode (either the first 524 or the second electrode 526) and generate
`
`secondary electrons (not shown) from that electrode. The magnetic fields 508a,
`
`508b confine many of the electrons 426 and the secondary electrons in the
`
`
`
`2
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`

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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`chamber 502 thereby improving the efficiency of the excitation process in the
`
`chamber 502.
`
` Iwamura, in contrast, does not mention a magnet nor metastable
`
`atoms. Indeed, the Petitioner’s own expert, Dr. Kortshagen, admitted in his
`
`deposition that he could not find any mention of either a magnet or metastable
`
`atoms in Iwamura:
`
`Q. In your opinion, is there any explicit reference to metastable
`
`atoms in the Iwamura patent?
`
`A. Explicit in the term that it -- it says metastable atom, I don't
`
`think there is; that is correct.2
`
`…
`
`A. No, Iwamura actually does not disclose a magnet, and this is
`
`why in the declaration referring to claim 18, which maybe you
`
`could hand me a little later, we're invoking obviousness over
`
`Iwamura and Angelbeck and Pinsley.3
`
`But Angelbeck and Pinsley cannot possibly compensate for the deficiencies of
`
`Iwamura because as explained by the Patent Owner’s expert Dr. Hartsough,
`
`“Angelbeck’s system produces a plasma, not excited/metastable atoms as
`
`claimed. Specifically, Angelbeck teaches, ‘[t]he current-excited discharge
`
`
`2 Exhibit 2004, Kortshagen Deposition (1.16.15), p. 105, ll. 4-9.
`
`3 Id. at p. 161, ll. 6-11.
`
`
`
`3
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`

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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`passed through the gas within tube 10 creates a plasma in which the atoms are
`
`ionized and electrons are freed.’”4 Moreover, as further explained by Dr.
`
`Hartsough, the magnetic fields disclosed in Angelbeck and Pinsley would
`
`create a transverse magnetic field increasing the loss of electrons to the tube
`
`walls, instead of trapping electrons proximate to the ground state atoms as
`
`claimed in the ‘779 patent.5
`
`Thus, Dr. Kortshagen’s conclusory opinions are unsupported and should
`
`be disregarded by the Board. Once the prior art is properly understood, the
`
`Board will see that it is missing key claim limitations, not only a “metastable
`
`atom source comprising a magnet that generates a magnetic field for
`
`substantially trapping electrons proximate to the ground state atoms,” but also
`
`many other limitations in the other claims of the ’779 patent as explained in
`
`detail below.6
`
`In addition to missing key limitations, the Petitioner’s obviousness
`
`rejections are all predicated on the false assumption that a skilled artisan could
`
`
`4 Exhibit 2005, Dr. Hartsough’s Declaration, ¶ 58, quoting Angelbeck, col. 2, ll.
`
`55-57.
`
`5 Id. at ¶ 60.
`
`6 Infra, § V.B.
`
`
`
`4
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`

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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`have achieved the combination of (i) a feed gas source comprising ground
`
`state atoms; (ii) an excited atom source that generates excited atoms from the
`
`ground state atoms and has a magnet that traps electrons near the ground state
`
`atoms; (iii) a plasma chamber that confines excited atoms; and (iv) an energy
`
`source that ionizes the confined excited atoms in a multi-step ionization
`
`process, as required by independent claims 1 and 18 of the ’779 patent by
`
`combining the teachings of Iwamura, Angelbeck, and Pinsley.7
`
`But these three references disclose very different structures and
`
`processes. As explained by Dr. Hartsough, the claimed invention of the ’779
`
`patent confines the excited atoms after they are transformed from ground state
`
`atoms so that they can later be ionized while the excited atoms in Angelbeck’s
`
`laser or Pinsley’s laser must return to their ground state to release energy so
`
`that the laser will operate according to its intended purpose: to emit light.8
`
`And the Petitioner sets forth no evidence that the structure and process
`
`of Iwamura would produce the particular plasma generator containing (i) a
`
`feed gas source comprising ground state atoms; (ii) an excited atom source that
`
`generates excited atoms from the ground state atoms and has a magnet that
`
`traps electrons near the ground state atoms; (iii) a plasma chamber that
`
`
`7 Petition at pp. 18-40.
`
`8 Exhibit 2005, Dr. Hartsough’s Declaration, ¶ 48.
`
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`5
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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`confines excited atoms; and (iv) an energy source that ionizes the confined
`
`excited atoms in a multi-step ionization process, as required by independent
`
`claims 1 and 18 of the ’779 patent if Iwamura were somehow modified by a
`
`structure that uses a laser to generate light like Angelbeck or Pinsley.9 Indeed,
`
`a laser emits light with the release of energy when electrons in atoms move to a
`
`lower energy state. Because higher energy atoms in Angelbeck and Pinsley’s
`
`laser are used to make light, they would not be available for the plasma
`
`generation process of Iwamura.
`
`That is, the Petitioner did not show that a “skilled artisan would have
`
`been motivated to combine the teachings of the prior art references to achieve
`
`the claimed invention, and that the skilled artisan would have had a reasonable
`
`expectation of success in doing so.”10 The Board has consistently declined to
`
`institute proposed grounds of rejections in IPR proceedings when the Petition
`
`fails to identify any objective evidence such as experimental data, tending to
`
`
`9 See e.g., Petition, pp. 18-40.
`
`10 OSRAM Sylvania, Inc. v. Am Induction Techs., Inc., 701 F.3d 698, 706 (Fed.
`
`Cir. 2012).
`
`
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`6
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`

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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`establish that two different structures or processes can be combined.11 Here,
`
`the Petitioner did not set forth any such objective evidence.12
`
`For these reasons as expressed more fully below, none of the challenged
`
`claims of the ‘779 patent are obvious.
`
`
`
`II. TECHNOLOGY BACKGROUND
`
`A. Overview Of Plasma Generation
`
`“A plasma is a collection of charged particles that move in random
`
`directions.”13 “For example, a plasma can be generated by applying a
`
`potential of several kilovolts between two parallel conducting electrodes in an
`
`inert gas atmosphere (e.g., argon) at a pressure that is between about 10-1 and
`
`10-2 Torr.”14 Plasma is generated for use in sputtering systems, which deposit
`
`films on substrates:
`
`Ions, such as argon ions, are generated and are then drawn out of
`
`the plasma and accelerated across a cathode dark space. The target
`
`
`11 Epistar, et al. v. Trustees Of Boston University, IPR2013-00298, Decision Not To
`
`Institute, Paper No. 18 (P.T.A.B. November 15, 2103).
`
`12 See e.g., Petition, pp. 14-60.
`
`13Exhibit 1301, ‘779 patent col. 1, ll. 7-9.
`
`14 Id. at col. 1, ll. 14-16.
`
`
`
`7
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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`surface has a lower potential than the region in which the plasma
`
`is formed. Therefore, the target surface attracts positive ions.
`
`Positive ions move towards the target with a high velocity and
`
`then impact the target and cause atoms to physically dislodge or
`
`sputter from the target surface. The sputtered atoms then
`
`propagate to a substrate or other work piece where they deposit a
`
`film of sputtered target material.15
`
`Magnets can be used in sputtering systems to increase the deposition rate:
`
`Magnetron sputtering systems use magnetic fields that are shaped
`
`to trap and concentrate secondary electrons proximate to the target
`
`surface. The magnetic fields increase the density of electrons and,
`
`therefore, increase the plasma density in a region that is proximate
`
`to the target surface. The increased plasma density increases the
`
`sputter deposition rate.16
`
`These magnetron sputtering systems, however, have “undesirable non-
`
`uniform erosion of target material.”17 To address these problems, researchers
`
`increased the applied power and later pulsed the applied power.18 But
`
`increasing the power increased “the probability of establishing an electrical
`
`
`15 Id. col. 1, ll. 30-42.
`
`16 Id. at col. 1, ll. 50-57.
`
`17 Id. at col. 4, ll. 64-65.
`
`18 Id. at col. 4, ll. 3-20.
`
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`8
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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`breakdown condition leading to an undesirable electrical discharge (an
`
`electrical arc) in the chamber.”19 And “very large power pulses can still result
`
`in undesirable electrical discharges and undesirable target heating regardless of
`
`their duration.”20
`
`B. The ’779 patent: Dr. Chistyakov invents a new plasma generator
`containing a feed gas source, an excited atom source with a magnet that
`traps electrons, a plasma chamber that confines excited atoms, and an
`energy source that ionizes the confined excited atoms in a multi-step
`ionization process.
`
`To overcome the problems of the prior art, Dr. Chistyakov invented a
`
`plasma generator containing (i) a feed gas source comprising ground state
`
`atoms; (ii) an excited atom source that generates excited atoms from the
`
`ground state atoms and has a magnet that traps electrons near the ground state
`
`atoms; (iii) a plasma chamber that confines excited atoms; and (iv) an energy
`
`source that ionizes the confined excited atoms in a multi-step ionization
`
`process as recited in independent claims 1 and 18 and as illustrated in Fig. 2 of
`
`the ’779 patent, reproduced below:
`
`
`19 Id. at col. 4, ll. 7-9.
`
`20 Id. at col. 4, ll. 18-20.
`
`
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`9
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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`
`
`
`
`As illustrated by FIG. 2, Dr. Chistyakov’s plasma generation apparatus
`
`includes “an excited atom source that generates excited atoms from ground
`
`state atoms from a feed gas source 206.”21 In one embodiment, “the excited
`
`atom source is a metastable atom source 204.”22 “The feed gas source 206
`
`provides a volume of ground state atoms 208 to the metastable atom source
`
`204.”23 “The plasma generator of the present invention can use any type of
`
`
`21 Id. at col. 4, ll. 30-31.
`
`22 Id. at col. 4, ll. 31-34.
`
`23 Id. at col. 4, ll. 34-36.
`
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`10
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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`metastable atom source 204. Skilled artisans will appreciate that there are
`
`many methods of exciting ground state atoms 208 to a metastable state.”24
`
`Dr. Chistyakov’s plasma generation apparatus then moves the excited or
`
`metastable atoms toward a chamber:
`
`The plasma chamber 230 confines the volume of metastable atoms
`
`218. In one embodiment, the output of the metastable atom source
`
`204 is positioned so as to direct the volume of metastable atoms
`
`218 towards the cathode assembly 114. In one embodiment, the
`
`geometry of the plasma chamber 230 and the cathode assembly
`
`114 is chosen so that the metastable atoms reach the cathode
`
`assembly 114 at a time that is much less than an average transition
`
`time of the metastable atoms to ground state atoms.25
`
`The plasma generator also includes a magnet to increase the plasma density
`
`near the cathode:
`
`In one embodiment, a magnet (not shown) is disposed proximate
`
`to the cathode assembly 114. The magnet generates a magnetic
`
`field that traps electrons in the plasma proximate to the cathode
`
`assembly 114 and, therefore, increases the plasma density. In the
`
`region proximate to the cathode assembly 114.26
`
`
`24 Id. at col. 5, ll. 1-5.
`
`25 Id. at col. 6, ll. 48-56.
`
`26 Id. at col. 6, ll. 34-39.
`
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`11
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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`“The plasma generator 200 of FIG. 2 uses a multi-step or stepwise
`
`ionization process to generate the plasma 202.”27 A “multi-step ionization
`
`process according to the present invention includes a first step where atoms are
`
`excited from a ground state to an excited state and a second step where atoms
`
`in the excited state are ionized.”28
`
`Dr. Chistyakov’s “multi-step ionization process … substantially
`
`increases the rate at which the plasma 202 is formed and therefore, generates a
`
`relatively dense plasma.”29 “Once a plasma having the desired characteristics
`
`is generated, the plasma 202 can be used in the processing of the workpiece
`
`138. … In a plasma sputtering application, ions in the plasma can be used to
`
`sputter material from the target 116. The sputtered material is deposited on the
`
`workpiece 138 to form a thin film.”30
`
`Thus, Dr. Chistyakov accomplished his breakthrough of improve plasma
`
`generation by inventing a particular apparatus comprising (i) a feed gas source
`
`comprising ground state atoms; (ii) an excited atom source that generates
`
`excited atoms from the ground state atoms and has a magnet that traps
`
`
`27 Id. at col. 6, ll. 60-61.
`
`28 Id. at col. 7, ll. 4-7.
`
`29 Id. at col. 8, ll. 65-67.
`
`30 Id. at col. 9, ll. 42-50.
`
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`12
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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`electrons near the ground state atoms; (iii) a plasma chamber that confines
`
`excited atoms; and (iv) an energy source that ionizes the confined excited
`
`atoms in a multi-step ionization process. In the claimed invention of the ‘779
`
`patent, ground state atoms are transformed to excited atoms and the excited
`
`atoms are moved to a plasma chamber where they are confined and ionized by
`
`an energy source.
`
`C. The Petitioners Mischaracterized The File History.
`
`The Petitioners alleged that the claims of the ’779 patent were allowed
`
`solely because the Applicant (i.e., now the Patent Owner) “amended the
`
`independent claims at issue here to require that the distinct source further
`
`includes ‘a magnet that generates a magnetic field for substantially trapping
`
`electrons proximate to the ground state atoms.’”31
`
`But this allegation is not true because the Applicant amended the
`
`independent claims to specify that “an excited atom source receives ground
`
`state atoms from the feed gas source.”32 More important, the Applicant
`
`amended the claims at the suggestion of the Examiner to include the
`
`limitations from a dependent claim, as applicants frequently do.33 That is, the
`
`
`31 Petition, p. 11 (citing Ex. 1309, 05/06/04 Resp. at 2, 4, 6, 8 and 10).
`
`32 Exhibit 1309, 05/06/04 Resp. at 2.
`
`33 Id. at 11.
`
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`13
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`IPR2014-00829
`U.S. Patent No. 6,805,779
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`independent claims were allowed because of all the components recited within
`
`them (i.e., the feed gas source, excited atom source, plasma chamber, energy
`
`source) as well as the recitation of the transformation of ground state atoms to
`
`excited atoms and the movement of the excited atoms among the various
`
`components, and not because of one of the claim amendments made prior to
`
`allowance of the patent.
`
`
`
`
`
`III. SUMMARY OF THE INSTITUTED GROUNDS FOR REVIEW
`
`For the Board’s convenience below is a summary of the proposed
`
`grounds of rejection instituted in this IPR proceeding:
`
`1. Claims 16, 28, 41, 42, and 45: obvious in view of the combination
`
`of Iwamura, Angelbeck, and Pinsley;
`
`2. Claim 46: anticipated by Iwamura.
`
`
`
`IV. CLAIM CONSTRUCTION.
`
`Under the Board’s rules, any unexpired claim “shall be given its broadest
`
`reasonable construction in light of the specification of the patent in which it
`
`appears.”34 Under that construction, claim terms are to be given their ordinary
`
`
`34 37 C.F.R. § 42.100(b).
`
`
`
`14
`
`

`
`IPR2014-00829
`U.S. Patent No. 6,805,779
`
`and customary meaning as would be understood by one of ordinary skill in the
`
`art in the context of the entire patent disclosure.35 The customary meaning
`
`applies unless the specification reveals a special definition given to the claim
`
`term by the patentee, in which case the inventor’s lexicography governs.36 Any
`
`term not construed below should be given its ordinary and customary meaning
`
`as would be understood by one of ordinary skill in the art.
`
`
`
`A. The construction of “metastable atoms,” “multi step ionization,” and
`“excited atoms.”
`
`The Board construed “metastable atoms” as “excited atoms having
`
`energy levels from which dipole radiation is theoretically forbidden.”37 The
`
`Board also construed the claim term “multi-step ionization” as “an ionization
`
`
`35 Phillips v. AWH Corp., 415 F.3d 1303, 1313 (Fed. Cir. 2005) (en banc);
`
`Research in Motion v. Wi-Lan, Case IPR2013-00126, Paper 10 at 7 (P.T.A.B.
`
`June 20, 2013).
`
`36 See Phillips, 415 F.3d at 1316 (“[T]he specification may reveal a special
`
`definition given to a claim term by the patentee that differs from the meaning
`
`that it would otherwise possess. In such cases, the inventor’s lexicography
`
`governs.”).
`
`37 IPR2014-00828, Institution Decision, Paper No. 9, p. 8.
`
`
`
`15
`
`

`
`process having at least two distinct steps.”38 The Board construed the claim
`
`term “excited atoms” as “atoms that have one or more electrons in a state that
`
`IPR2014-00829
`U.S. Patent No. 6,805,779
`
`is higher than its lowest possible state.”39
`
`
`
`B.
`
` The construction of the means plus function limitations
`
`A means plus function "claim [limitation] shall be construed to cover the
`
`corresponding structure, material, or acts described in the specification and
`
`equivalents thereof."40 I understand that the Board construed the means plus
`
`function limitations appearing in the claims of the ‘779 patent as follows:41
`
`Recited functions in italics
`
`Corresponding structures
`
`means for generating a
`
`magnets—e.g., magnets
`
`566a-d,
`
`magnetic field proximate to a
`
`570a-d, 712, 714 that generate a
`
`volume of ground state
`
`magnetic field as shown in Figures 7,
`
`atoms to substantially trap
`
`7A, and 10 of the ’779 patent. See Ex.
`
`electrons proximate to the
`
`1301, 16:1–20 (“The magnets 566a-d,
`
`volume of ground state
`
`570a-d create a magnetic field 574 that
`
`atoms (claim 41)
`
`substantially
`
`traps and accelerates
`
`electrons (not shown) in the chamber
`
`
`38 Id. at 10.
`
`39 IPR2014-00829, Institution Decision, Paper No. 9, p. 7.
`
`40 35 U.S.C. § 112, ¶ 6.
`
`41 IPR2014-00829, Institution Decision, Paper No. 9, p. 12.
`
`
`
`16
`
`

`
`IPR2014-00829
`U.S. Patent No. 6,805,779
`
`554.”), 18:34–41, Figs. 7, 7A, 10.
`
`means for generating a
`
`a metastable atom source—e.g.,
`
`volume of metastable atoms
`
`metastable atom sources 402, 450,
`
`from the volume of ground
`
`500, 550, 600, 650, 700, 735 as shown
`
`state atoms (claim 41)
`
`in Figures 4–11 of the ’779 patent. Ex.
`
`1301, 14:24–26, 14:46–48, 15:46–
`
`67, 16:29–31, 17:27–34, 18:7–16,
`
`19:11–12.
`
`means for raising an energy
`
`a power supply generating an electric
`
`of the metastable atoms so
`
`field between a cathode assembly and
`
`that at least a portion of the
`
`an anode as shown in Figures 2 and 3
`
`volume of metastable atoms
`
`of the ’779 patent. Ex. 1301, 8:39–5,
`
`is ionized, thereby
`
`11:4–14.
`
`generating a plasma with a
`
`multistep ionization process
`
`(claim 41)
`
`means for trapping electrons
`
`an
`
`electron
`
`ion/absorber—e.g.,
`
`and ions in the volume of
`
`electron ion/absorbers 536, 618, 664,
`
`metastable atoms (claim 42)
`
`728, 750, 750’, and 750” shown in
`
`Figures 6, 8, 9, 10, and 12A–12C of
`
`the ’779 patent. Pet. 19; Ex. 1301,
`
`14:66–15:9, 16:56–62, 17:35–42,
`
`18:42–67, 19:56–20:32.
`
`
`
`
`
`17
`
`

`
`IPR2014-00829
`U.S. Patent No. 6,805,779
`
`V. THE PETITIONERS CANNOT PREVAIL ON ANY CHAL

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