`U.S. Patent No. 7,110,444
`Patent Owner’s Sur-Reply
`
`
`
`UNITED STATES PATENT AND TRADEMARK OFFICE
`
`____________________________
`
`BEFORE THE PATENT TRIAL AND APPEAL BOARD
`
`____________________________
`
`Intel Corporation
`Petitioner
`v.
`
`ParkerVision, Inc.
`Patent Owner
`
`U.S. Patent No. 7,110,444
`
`Issue Date: September 19, 2006
`Title: WIRELESS LOCAL AREA NETWORK (WLAN) USING UNIVERSAL
`FREQUENCY TRANSLATION TECHNOLOGY INCLUDING MULTI-PHASE
`EMBODIMENTS AND CIRCUIT IMPLEMENTATIONS
`__________________________________________________________________
`
`Inter Partes Review No. IPR2020-01265
`__________________________________________________________________
`
`PATENT OWNER’S SUR-REPLY TO PETITIONER’S REPLY
`
`
`
`TABLE OF CONTENTS
`
`
`Page
`
`INTRODUCTION ........................................................................................... 1
`
`INTEL’S EXPERT MAKES CRITICAL ADMISSIONS AGAINST
`INTEL’S POSITION ....................................................................................... 3
`
`I.
`
`II.
`
`III. TAYLOE’S SYSTEM IS FUNDAMENTALLY DIFFERENT THAN
`PARKERVISION’S CLAIMED INVENTION. ............................................. 6
`
`IV. PARKERVION’S CONSTRUCTION IS BASED ON HOW
`TECHNOLOGY ACTUALLY WORK; INTEL RELIES ON A NAMING
`CONVENTION ............................................................................................... 8
`
`V.
`
`THE TEXAS COURT’S UPDATED CONSTRUCTION ............................ 10
`
`VI.
`
`INTEL’S CONSTRUCTION OF “STORAGE ELEMENT” IS WRONG. . 10
`
`A. A “Storage Element” Is Only an Element of an Energy Transfer
`System. ................................................................................................ 10
`
`B.
`
`A “Storage Element” Drives a Low Impedance Load. ........................ 13
`
`VII. TAYLOE DOES NOT DISCLOSE A “STORAGE ELEMENT” ................ 14
`
`A.
`
`Intel Admits That a “Storage Element” Stores Non-Negligible
`Amounts of Energy. ............................................................................ 14
`
`B.
`
`The Capacitors in Tayloe Hold Negligible Amounts Of Energy. ....... 17
`
`1.
`
`Energy in a Tayloe Capacitor. .................................................. 18
`
`a.
`
`b.
`
`c.
`
`STEP 1: Calculating available energy. ........................... 18
`
`STEP 2: Calculating energy in capacitor. ....................... 21
`
`STEP 3: Percentage of available energy. ....................... 22
`
`2.
`
`Energy in ParkerVision’s storage element. ............................... 23
`
`a.
`
`STEP 1: Calculating available energy. ........................... 23
`
`
`
`i
`
`
`
`b.
`
`c.
`
`STEP 2: Energy stored on storage element. ................... 24
`
`STEP 3: Percentage of available energy. ....................... 25
`
`C.
`
`Tayloe Does Not Disclose An Energy Transfer System. .................... 25
`
`
`
`
`
`
`ii
`
`
`
`I.
`
`INTRODUCTION
`
`First, while the parties’ constructions of “storage element” are different, the
`
`parties agree that a “storage element” must store non-negligible amounts of energy
`
`from an input electromagnetic (EM) signal. The capacitors of Tayloe (Intel’s
`
`primary reference), however, only hold a negligible (near zero) amount of energy
`
`from an input EM signal. No other Intel prior art reference changes this fact.
`
`In particular, using the values provided in Tayloe, a capacitor in Tayloe holds
`
`only 0.193% of the energy from an input EM signal – a negligible amount of energy.
`
`On the other hand, using the values provided in the ’444 patent (which incorporates
`
`the ’551 patent) for an energy transfer embodiment, a storage element stores 58.7%
`
`of the energy from an input EM signal – a non-negligible amount of energy. See
`
`Section VII.B. For at least this reason, challenged claim 3 is not invalid.
`
`Recognizing that Tayloe does not disclose storing non-negligible amounts of
`
`energy from an input EM signal, Intel provides only a superficial discussion of this
`
`critical issue. Tellingly, Intel quickly shifts its discussion away from energy storage
`
`and, instead, focuses on a control signal having non-negligible aperture widths. But
`
`whether a control signal has non-negligible apertures does not mean that a capacitor
`
`will store non-negligible amounts of energy from an input EM signal. How much
`
`energy is stored depends on the specific components/configuration of a system.
`
`
`
`1
`
`
`
`Second, the parties dispute whether a “storage element” is an element of an
`
`“energy transfer system.” In its Response, ParkerVision explained why it is. See
`
`Paper 18 (“POR”), 46-50. The Texas District Court (“Texas Court”) has now twice
`
`agreed with ParkerVision.1 Yet, before this Board, Intel persists in making the exact
`
`same flawed arguments that it made to the Texas Court – arguments which rely on a
`
`mere naming convention rather than how the technology is actually described in the
`
`patent, and which the Texas Court has twice rejected.
`
`Indeed, the negligible amount of energy held in a Tayloe capacitor is exactly
`
`what one would expect in a voltage sampling system, not an energy transfer system
`
`(a system which drives a low impedance load). Thus, the capacitors of Tayloe are
`
`not “storage elements.” For this additional reason, challenged claim 3 is not invalid.
`
`Finally, the parties dispute whether an energy transfer system is driving a low
`
`impedance load. Intel incorrectly asserts that limiting the construction in this way is
`
`inconsistent with the specification. See Reply, 3-4. To the contrary, the specification
`
`specifically states that driving a low impedance load is a “benefit” of an energy
`
`
`1 That the Texas Court twice provided constructions that support ParkerVision’s
`
`view of “storage element” (see Ex.-2012, 4-5; Ex.-1038, 2) belies Intel’s assertion
`
`that ParkerVision’s arguments lack support in law or fact. See Paper 21 (“Reply”),
`
`4.
`
`2
`
`
`
`transfer system. Indeed, after ParkerVision filed its POR, in a second litigation
`
`against Intel, the Texas Court once again considered the term “storage module”2 in
`
`a related ParkerVision patent and expressly included the language “for driving a low
`
`impedance load” in its construction. This supports ParkerVision's interpretation of
`
`(and provides clarification regarding) what it means for a system to be an “energy
`
`transfer system.”
`
`Tayloe, however, discloses a high impedance load, not a low impedance load.
`
`And as discussed in Section VII.D below, Tayloe does not deliver enough energy to
`
`a load to drive a low impedance load. For this additional reason, challenged claim 3
`
`is not invalid.
`
`II.
`
`INTEL’S EXPERT MAKES CRITICAL ADMISSIONS AGAINST
`INTEL’S POSITION
`
`Intel asserts that Tayloe discloses an “energy transfer system” because the
`
`summing amplifiers 50, 52 in Tayloe are low impedance loads. Reply, 26-27. Intel’s
`
`expert, Dr. Subramanian, however, effectively concedes that these summing
`
`amplifiers are actually high impedance loads.
`
`First, in both of his declarations, Dr. Subramanian admits that Tayloe’s
`
`summing amplifiers use operational amplifiers (op-amps). See Ex.-1002, ¶138 (“the
`
`
`2 Intel agrees that the terms “storage element” and “storage module” are used
`
`interchangeably. Reply, 10 n. 2.
`
`3
`
`
`
`triangular element depicted within the amplifier 50 [of Tayloe] … is an operational
`
`amplifier.”);3 Ex.-1030, ¶¶17-21. Operational amplifiers are high impedance loads.
`
`Ex.-2021, ¶¶90, 263-265. Indeed, during his deposition, Dr. Subramanian admitted
`
`that (1) with regard to input impedance “the ideal OP amp is assumed to be infinite,
`
`but in reality, it starts at the meg[]ohm typically and goes up from there.” (Ex.-2028,
`
`170:15-18) and (2) the most widely sold commercial op-amp at the time (the 741
`
`series) typically had an input impedance of about 1 megohm. Ex.-2028, 138:21-
`
`139:18. One megohm is a high impedance load as discussed below.
`
`Notably, Dr. Subramanian’s testimony is consistent with Figure 78A of the
`
`’551 patent (below) (a voltage sampling system), which shows 1 megohm as a high
`
`impedance load.
`
`
`3 Unless otherwise notes, all emphasis has been added.
`
`4
`
`
`
`
`
`Dr. Subramanian’s only basis for asserting that there is a low impedance
`
`presented at the input of Tayloe’s op-amp is the presence of a resistor before the op-
`
`amp. Ex.-1030, ¶16. According to Dr. Subramanian, there would be no need to
`
`include a resistor in the circuit if the impedance of the non-inverting input (+) of the
`
`op-amp were high. Id., ¶18. Critically, at his deposition, Dr. Subramanian
`
`contradicted his declaration and ultimately admitted that the resistor before the
`
`Tayloe op-amp serves another purpose – a compensation resistor. See Ex.-2028,
`
`154:4-16. A compensation resistor is put before an op-amp in order to eliminate
`
`voltage offsets (i.e., to eliminate the errors that would be introduced by input bias
`
`currents). Ex.-2028 184:9-185:6. As such, Dr. Subramanian’s deposition testimony
`
`5
`
`
`
`eliminated his only basis as to why he viewed the op-amp as presenting a low
`
`impedance load.
`
`III. TAYLOE’S SYSTEM IS FUNDAMENTALLY DIFFERENT THAN
`PARKERVISION’S CLAIMED INVENTION.
`
`Tayloe is a voltage sampling system – a fundamentally different and
`
`competing technology to ParkerVision’s energy transfer (energy sampling) system.
`
`Intel seeks to ignore the distinction between an energy transfer system
`
`(ParkerVision’s claimed invention), which uses a “storage element” (the term at
`
`issue here), and a voltage sampling system (Tayloe), which uses a “holding element”
`
`(a different term used in the ’444 patent). See POR, 19-22, 33-42, 47-50.
`
`In an energy transfer system, the energy stored in a “storage element”
`
`becomes part of (is incorporated into) the down-converted signal (as a result of the
`
`
`
`6
`
`
`
`energy being transferred to and driving a low impedance load). See Ex.-2021, ¶¶160,
`
`165, 168, 173. Since the flow of energy itself forms the down-converted signal, the
`
`storage element must store non-negligible amounts of energy. Id., ¶200.
`
`Tayloe is different – i.e., Tayloe is not including energy from a capacitor in
`
`the down-converted signal. Instead, Tayloe is only holding energy in a capacitor in
`
`order to take readings of voltage.4 As such, the ’444 patent refers to this type of
`
`element as a “holding element.” The readings are, in turn, used to accurately
`
`reproduce the voltage of the input signal in order to create a down-converted signal.
`
`Since Tayloe is simply capturing a voltage measurement, a Tayloe capacitor
`
`only holds negligible amounts of energy (near zero). Moreover, in order to hold
`
`energy in a capacitor long enough to take a measurement, Tayloe uses a high
`
`impedance load which prevents energy in the capacitor from being discharged from
`
`the capacitor into the load. As a result, the capacitors in Tayloe do not drive a low
`
`
`4 A voltage sampling system seeks to accurately represent the voltage of the input
`
`signal. It does so by holding the voltage value on a capacitor. Unlike voltage
`
`sampling, energy sampling systems cannot accurately represent the voltage of the
`
`input signal because a non-negligible amount of energy in the storage element is
`
`being transferred to a low impedance load, even between samples. See, e.g., Ex.-
`
`2021, ¶164.
`
`7
`
`
`
`impedance load. These features of Tayloe are all features of a voltage sampling
`
`system.
`
`IV. PARKERVION’S CONSTRUCTION
`IS BASED ON HOW
`TECHNOLOGY ACTUALLY WORK; INTEL RELIES ON A
`NAMING CONVENTION
`
`Intel asserts that ParkerVision is attempting to redefine what the ’444 patent
`
`says about the patented technology. Reply, 3. Not so.
`
`Unlike ParkerVision, who focuses on how the technology actually works,
`
`Intel relies on a naming convention used in the patent to push a flawed narrative –
`
`one that has twice been rejected by the Texas Court. See Reply, 2-3, 6-8. In
`
`particular, Intel points out that the ’444 patent (which incorporates the ’551 patent)
`
`refers to the two distinct systems for down-conversion – “under-sampling” systems
`
`and “energy transfer” systems.5 Id., 6-8. Intel then complains that ParkerVision
`
`describes “under-sampling” systems as “voltage sampling/sample and hold” and
`
`“energy transfer” systems as “energy sampling/energy transfer.” Id., 4. But that is
`
`
`5 Intel’s discussion of “aliasing rate” is inapplicable. See Reply, 5-6. Aliasing rate is
`
`simply the rate at which an input signal is sampled. It is not what distinguishes an
`
`“under-sampling” system and an “energy transfer” system.
`
`8
`
`
`
`exactly what they are. The fact that the patent does not use the terms “voltage
`
`sampling” and “energy sampling” verbatim is beside the point.6
`
`In particular, the ’444 patent relates to the use of sampling to down-convert a
`
`signal and teaches only two things that can be sampled to down-convert a signal: (1)
`
`voltage and (2) flow of energy over time. Voltage is sampled by taking and holding
`
`input voltage values (using a “holding” element).7 On the other hand, energy is
`
`sampled by transferring non-negligible amounts of energy from an input signal. See,
`
`e.g., Ex.-2007, 63:27-30. As such, there are only two systems that can sample to
`
`down-convert a signal – the same two systems discussed in the patent: (1) “voltage”
`
`sampling system (referred to as “under-sampling systems”) and (2) “energy”
`
`sampling system (referred to as “energy transfer” systems). Compare Ex.-2007,
`
`64:20-50 (describing an “under-sampling system”) with 66:55-68:13 (describing an
`
`
`6 Intel’s reliance on the timing diagrams (Figures 83E-F) of the ’551 patent – which
`
`plot measurements of voltage instead of energy over time – is of no moment. Energy
`
`cannot be measured directly. Instead, a measurement (voltage or its inverse, current)
`
`needs to be taken from which energy can be derived. See Ex.-1030, ¶7.
`
`7 The ’551 patent specifically discloses that “[t]he under-sampling systems utilize a
`
`sample and hold system controlled by an under-sampling signal.” Ex.-2007, 63:4-5.
`
`A sample and hold system is a “voltage sampling” system. Ex.-2021, ¶142.
`
`9
`
`
`
`“energy transfer system”). This is the reason why ParkerVision’s POR refers to
`
`voltage sampling systems and energy sampling systems.
`
`V. THE TEXAS COURT’S UPDATED CONSTRUCTION
`
`Since ParkerVision filed its POR, the Texas Court revisited its construction
`
`of “storage module” (which the parties agree is synonymous with “storage element”)
`
`in a related patent. See Ex.-1038, 2. The Texas Court construed “storage module” as
`
`“a module of an energy transfer system that stores non-negligible amounts of energy
`
`from an input electromagnetic signal for driving a low impedance load.” Id.
`
`The Texas Court’s addition of “for driving a low impedance load” to its
`
`original construction supports ParkerVision’s interpretation of (and provides
`
`clarification regarding) what it means for a system to be an “energy transfer system”
`
`as set forth in ParkerVision’s proposed construction of “storage element.” See POR,
`
`49-50.
`
`VI.
`
`INTEL’S CONSTRUCTION OF “STORAGE ELEMENT” IS WRONG.
`
`The Texas Court has now twice considered and rejected Intel’s construction
`
`and arguments. While the Board is not bound to the Texas Court’s construction, it is
`
`informative.
`
`A. A “Storage Element” Is Only an Element of an Energy Transfer
`System.
`
`The ’444 patent specification (which incorporates the ’551 patent) states that
`
`the “energy transfer” system uses “a storage module” that “stores non-negligible
`
`10
`
`
`
`amounts of energy,” whereas the “under-sampling” (i.e., sample-and-hold) system
`
`utilizes a “holding module” that “stores negligible amounts of energy.” Ex.-2007.
`
`66:55-67. As such, there should be no dispute that “energy transfer system” should
`
`be included in the construction as ParkerVision proposes.
`
`Tellingly, Intel provides no substantive technical arguments based on the
`
`intrinsic evidence as to why including “an element of an energy transfer system” is
`
`technically incorrect. Instead, Intel points to a single sentence from the specification
`
`(red below)8 and asserts that this passage is enough to define the “storage” element.9
`
`It is not.
`
`FIG. 82A illustrates an exemplary energy transfer system 8202 for
`
`down-converting an input EM signal 8204. The energy transfer system
`
`8202 includes a switching module 8206 and a storage module
`
`illustrated as a storage capacitance 8208. The terms storage module
`
`and storage capacitance, as used herein, are distinguishable from the
`
`terms holding module and holding capacitance, respectively. . . .
`
`
`8 Notably, Intel never asserts that this red passage provides lexicography for “storage
`
`element.”
`
`9 Intel asserts that the goal of storage module is to store non-negligible amounts of
`
`energy. See Reply, 10. While storage of non-negligible amounts of energy is
`
`certainly one goal, it is not the only goal nor is this feature the only thing that defines
`
`what it means to be a “storage” element.
`
`11
`
`
`
`Storage modules and storage capacitances, on the other hand, refer to
`
`systems that store non-negligible amounts of energy from an input EM
`
`signal.
`
`Ex.-2007, 66:55-67.
`
`
`The entire paragraph above is describing a “storage” module/element in the
`
`context of an energy transfer system (green above), which is the only type of system
`
`that has a “storage” module/element. Indeed, this passage is found in the section
`
`entitled “0.1.2 Introduction to Energy Transfer.” See Ex.-2007, 66:33. As such, there
`
`is no basis for Intel to argue against including “energy transfer system.”
`
`The inclusion of “energy transfer system” in “storage element” is appropriate.
`
`First, in its Reply, Intel admits that there are only two systems disclosed in the
`
`patent: (1) energy transfer and (2) under-sampling. Reply, 6. Second, the ’444 patent
`
`states that a “storage” element is only used in an energy transfer system. Ex.-2007,
`
`66:55-59. Logically, if there are only two systems and a “storage” element is only
`
`used in an energy transfer system, then a “storage” module/element must necessarily
`
`be an element of an energy transfer system. Indeed, the specification makes it clear
`
`that “storage” modules/elements are inseparably intertwined with energy transfer
`
`systems. See POR, 46-50.
`
`Further, Intel argues that Intel’s construction of “storage element” is the same
`
`as ParkerVision’s proposed construction of “storage module” in a previous IPR
`
`(IPR2014-00948). Reply, 11-12. But this cuts against Intel’s argument. In 2014,
`
`12
`
`
`
`claim terms were interpreted according to their broadest reasonable interpretation
`
`(BRI) – a different standard than the Board uses today. In 2018, the USPTO
`
`eliminated the BRI standard and harmonized its claim construction standard with the
`
`district courts. In IPR2014-00948, ParkerVision focused on the red passage above.
`
`The PTAB’s current claim construction standard, however, requires considering
`
`more than just the red passage, which ParkerVision has done here.
`
`B. A “Storage Element” Drives a Low Impedance Load.
`
`A “low impedance load” goes to the heart of what makes an element, a
`
`“storage” element (used in energy sampling) as opposed to a “holding” element
`
`(used in voltage sampling/sample-and-hold). Unlike a low impedance load, a high
`
`impedance load causes an element to “hold” energy, making it a “holding” element,
`
`not a “storage” element.10 This is the reason the specification specifically makes a
`
`point to say that a “holding” modules/elements hold “negligible amounts of
`
`energy…with the intent of ‘holding’ a voltage value.’” Ex.-2007, 66:63-65. Intel
`
`does not address this language.11
`
`
`10 A high impedance load restricts the flow of current. Ex.-2007, 64:21-30. A low
`
`impedance load provides little resistance to electrical current. Ex.-2021, ¶200 n. 11.
`
`11 Intel asserts that the Texas Court did not include “driving a low impedance load”
`
`in its original construction. Reply, 15. Such a position is moot. Not only is “driving
`
`13
`
`
`
`Indeed, the way in which “holding” modules/elements “hold” a voltage value
`
`is by using a high impedance load. See, e.g., Ex.-2021, ¶148. As such, a “storage”
`
`module/element is not using a high impedance load.
`
`So what type of load is a “storage” module/element using? The specification
`
`explains that with regard to loads, it is a binary choice – it is either high or low
`
`impedance: “Recall from the overview of under-sampling that loads can be
`
`classified as high impedance loads or low impedance loads.” Ex.-2007, 67:32-33.
`
`As such, because a “storage” module/element is not using a high impedance load, it
`
`must necessarily be using a low impedance load. This portion of the specification
`
`should not be ignored and, therefore, is included in ParkerVision’s construction.
`
`Finally, the specification states that in energy transfer systems driving a low
`
`impedance load is a benefit (it necessarily occurs). Id., 67:37-42.
`
`
`
`VII. TAYLOE DOES NOT DISCLOSE A “STORAGE ELEMENT”
`
`A.
`
`Intel Admits That a “Storage Element” Stores Non-Negligible
`Amounts of Energy.
`
`For the first time in its Reply, Intel defines “storage element.” It is now clear
`
`that the parties agree that a “storage element” must store non-negligible amounts of
`
`
`a low impedance load” implicit when referring to an “energy transfer system,” but
`
`the Texas Court has now expressly included this language. See Ex.-1038, 2.
`
`
`
`14
`
`
`
`energy from an input EM signal.12 Notably, however, Intel provides only a
`
`superficial analysis on this critical issue. See Reply, 19.
`
`Whether an element stores non-negligible amounts of energy, begs the
`
`question – “non-negligible” relative to what? Intel fails to address this issue. And
`
`without this proper context, Intel’s assessment of energy stored in Tayloe’s
`
`capacitors is meaningless. Thus, Intel fails to meet its burden of proving invalidity.
`
`The ’444 patent (by incorporating the ’551 patent) makes clear that “non-
`
`negligible” is relative to the available power (i.e., amount of energy available from
`
`the input EM signal). See, e.g., Ex.-2007, 67:14-22.
`
`Indeed, the parties agree that the storage element must store non-negligible
`
`amounts of energy “from an input electromagnetic (EM) signal.” As shown below,
`
`the input EM signal (blue) (and the energy it carries) is the signal received by a
`
`switch (orange). Id., 66:55-59, 67:14-30.
`
`
`12 Dr. Subramanian states the claims 198-202 of the ’551 patent, which recite
`
`integrating non-negligible amounts of energy, is the embodiment of Tayloe. Ex.-
`
`1030, ¶11. Not so. While Tayloe integrates, Tayloe integrates negligible amounts of
`
`energy. See Section VII.B.1.c.
`
`15
`
`
`
`
`
`
`
`As such, whether an element stores “non-negligible amounts of energy” is
`
`relative to the available energy of the input EM signal. Thus, in order to determine
`
`whether an element stores “non-negligible amounts of energy,” one needs to
`
`calculate the amount of energy that was available from the input EM signal during a
`
`sampling aperture and compare it to the amount of energy actually stored in an
`
`element during that sampling aperture. Only after determining this percentage can
`
`one determine if an element stores a non-negligible amount of energy. Intel fails to
`
`make these necessary calculations and, thus, does not meet its burden of proof.
`
`16
`
`
`
`Instead, for the first time in its Reply, Intel focuses on the size of Tayloe’s
`
`capacitor and that Tayloe’s capacitors accumulate energy over time.13 Rely, 19. But
`
`this superficial analysis provides no insight into whether a Tayloe capacitor stores
`
`non-negligible amounts of energy.
`
`B.
`
`The Capacitors in Tayloe Hold Negligible Amounts Of Energy.
`
`Unlike an energy transfer system, Tayloe works based on voltage. Thus, a
`
`Tayloe capacitor only holds negligible amounts of energy (near zero), because
`
`Tayloe is taking readings of voltage in a capacitor. See Section III.
`
`In order to determine whether an element stores “non-negligible amounts of
`
`energy” (Step 3 below), one needs to calculate the amount of energy that was
`
`available from the input EM signal during a sampling aperture (Step 1 below) and
`
`compare it to the amount of energy transferred to the element during that sampling
`
`
`13 Tellingly, Intel quickly shifts the focus from storage of non-negligible amounts of
`
`energy to Tayloe’s use of a control signal having a non-negligible aperture width.
`
`See Reply, 21. But that is not the relevant analysis.
`
`17
`
`
`
`aperture (Step 2 below). When presented with the formulas of Steps 1-3, Dr.
`
`Subramanian agreed that those are the correct formulas.14
`
`As shown below, the Tayloe system holds negligible (near zero) amounts
`
`energy – 0.193% of the available energy.15 For comparison, a ParkerVision storage
`
`element stores non-negligible amounts of energy – 58.7% of the available energy.
`
`1.
`
`Energy in a Tayloe Capacitor.
`
`a.
`
`STEP 1: Calculating available energy.
`
`In order to determine whether a non-negligible amount of energy is being
`
`transferred, one must first know the total amount of power available for transfer.
`
`
`14 See Ex.-2028, 26:21-27:21; 28:1-25; 29:5-31:22; 33:5-12, 17-22; 34:7-35:19;
`
`41:5-42:23; 43:6-44:13; 46:24-49:7; 49:12-24; 53:15-54:17; 54:22-56:13; 58:11-
`
`16; 64:19-66:8; Ex.-2022.
`
`15 Intel argues that Tayloe’s description of the capacitors as “integrators” “matches
`
`the ’551 patent’s description of a storage module’s operation,” and, thus, Tayloe’s
`
`capacitors operate in the same way. Reply, 19. Not so. While “charge builds up on
`
`[each] capacitor” during a separate quarter wave of the input signal, the Tayloe
`
`system transfers only a negligible amount of energy to each capacitor during a
`
`respective quadrant. See Section VII.B.1.c below; see also Ex.-2021, ¶¶263-365.
`
`
`
`18
`
`
`
`The maximum power transfer theorem is a fundamental theorem of circuits:
`
`This theorem states that when a source is connected to a load, maximum power is
`
`delivered to the load when the load resistance is equal to the internal source
`
`resistance. Intel’s expert agrees. Ex.-2028, 41:4-42:23; 109:18-111:6.
`
`Since the source being evaluating in Tayloe has an output resistance, the
`
`maximum energy (or power) that can be delivered to the load can be calculated by
`
`setting the load resistance equal to the source resistance. In his prior declaration,
`
`ParkerVision’s expert created a circuit diagram (below) to illustrate a single path of
`
`Figure 3 of Tayloe.16 The radio frequency source (dashed blue box) is what a
`
`POSITA would use to represent the input signal f1. Ex.-2021, ¶259.
`
`
`
`
`
`
`
`
`16 The circuit diagram and its analysis are applicable to each of the capacitors
`
`72,74,76,78 in Tayloe. Ex.-2021, ¶¶258, 262, 267.
`
`19
`
`
`
`A POSITA would model a source (an input EM signal) as having an ideal
`
`voltage source and a resistance RS in addition to RFILTER. See Ex-2021, ¶¶260-265;
`
`Ex.-1004, 4:46-49.
`
`The maximum power that can be delivered from the source (the available
`
`power from input EM signal) is obtained with RLOAD = RS. In “Experimental
`
`Results,” Tayloe discloses an embodiment of the product detector which was built
`
`as the direct conversion receiver 30 (in FIG. 3) utilizing an analog multiplexer and
`
`digital counter as shown in FIG. 7. Ex.-1004, 5:31-35.
`
`Considering an input signal with an available power of +10 dBm = 10
`
`milliwatts, this is the power delivered to RLOAD when RLOAD = RS = 50 ohms. Thus,
`
`the power delivered to the matched load, PMAX = 0.010 watts = 0.5 (VPEAK)2 / (RL) =
`
`(EPEAK)2 / (400) where EPEAK is the amplitude of the source. 17 Accordingly, the
`
`amplitude of EPEAK = 2 volts.
`
`Tayloe also describes the commutating switch connecting the input of the
`
`switch to an output at a rate of 7 MHz. Ex.-1004, 5:49-50 (“The prototyped direct
`
`conversion receiver has an input bandwidth of roughly 1 kHz centered at 7 MHz.”).
`
`The period (T) of a 7 MHz signal is mathematically calculated as the reciprocal of
`
`the frequency. The period of a 7 MHz signal is thus 142.86 nanoseconds. Since the
`
`
`17 When RL=RS, the peak of the sinusoidal voltage across is VPEAK = ½ EPEAK.
`
`20
`
`
`
`commutating switch in Tayloe connects the input to the output for a quarter cycle,
`
`the time the switch is closed is TON = T/4 = 35.71 nanoseconds = 35.71 ns. The
`
`switch is also off for 107.15 ns, during which time the voltage is held on the holding
`
`capacitor. Thus, the maximum amount of energy available from the input EM signal
`
`during TON is a product of the power delivered to a matched load and the time
`
`duration.
`
`As such, according to the experimental embodiment in Tayloe, the available
`
`energy during the time the switch is on is UTAYLOE = PL * TON = (0.010 W) * (35.71
`
`ns) = 35.71 * 10−11 J = 357.1 pJ = 357.1 pJ.
`
`b.
`
`STEP 2: Calculating energy in capacitor.
`
`When a step voltage VS is applied to a circuit consisting of a resistor and a
`
`capacitor, the voltage on the capacitor (VCAP) will increase from its initial starting
`
`value up to the voltage VS following an exponential curve. Ex-2028, 51:10-53:10;
`
`Ex. 2022, 14. If the starting voltage is 0 V, the capacitance value is C and the resistor
`
`value is R then VCAP = VS(1 – e–t/τ), where τ = RC is the time constant. Figure 4 of
`
`Tayloe illustrates how the system uses the input signal f1 to determine the voltage
`
`to which to charge each capacitor. Figure 4 shows a waveform 100 includes a signal
`
`125 corresponding to input signal f1. Ex.-2021, ¶¶252-256.
`
`Using Figure 4 of Tayloe, the ideal voltage source can be replaced by a
`
`constant voltage of EAVG = 1.800 V, or the voltage at point 110. See Ex.-2007, ¶¶255-
`
`21
`
`
`
`256 (comparing average value of the input signal f1 with peak voltage, EPEAK = 2.00
`
`V). The time constant in Tayloe is τTAYLOE,ON = (RS + RFILTER) * Cf = (50 + 50 Ω) *
`
`(0.3 µF) = 30 microseconds = 30 μs. The switch is on for TON = 35.71 ns. Thus, when
`
`the switch is closed, the voltage on Cf increases from 0 volts to a voltage VCAP =
`
`EAVG (1 – e–TON/τ) = EAVG * ( 1 – e–(35.71 ns/30 μs)) = EAVG * 0.001190. Now EAVG =
`
`1.800 V, so at the end of the charging interval VCAP = 0.002141 V. At the end of the
`
`charging interval, the energy held by the capacitor Cf is ECf = ½ C*(VCAP)2 = 0.5 *
`
`(0.3 μF) * (0.002141 V)2 = 6.878 * 10−13 J = 0.6878 pJ.
`
`c.
`
`STEP 3: Percentage of available energy.
`
`Having calculated the available energy (357.1 pJ) and the amount of energy
`
`held in a capacitor (0.6878 pJ), one can calculate the percentage of available energy
`
`that is held on Tayloe’s capacitor:
`
`0.6878 pJ = 0.193%
` 357.1 pJ
`
`As such, only 0.193% of the energy available is held on Tayloe’s capacitor
`
`Cf.18 This is a negligible (nearly zero) amount of energy. The balance of the energy
`
`
`18 Regardless of the number of apertures Tayloe uses, the percentage of energy held
`
`in a capacitor will always be the same because there is additional available energy
`
`during each aperture.
`
`22
`
`
`
`– 99.807% of the available energy – is not stored but, instead, is dissipated in the
`
`resistor RFILTER. Id., ¶264.
`
`2.
`
`Energy in ParkerVision’s storage element.
`
`a.
`
`STEP 1: Calculating available energy.
`
`Fig. 82B of the ’551 patent illustrates an exemplary energy transfer system.
`
`
`
`Similar to the Tayloe analysis above, annotated Fig. 82B of the ’551 patent
`
`
`
`incorporates an actual source (representing input EM signal) with RS = 50 ohms. The
`
`source voltage, E, is a sinusoidal signal with a peak value of 5 mV. See Ex.-2007,
`
`Fig. 83B. That is, EPEAK = 5 mV. The power available from the source =
`
`0.5*(EPEAK/2)2 / 50 = 62.5 nW. This energy sampling embodiment has an input signal
`
`centered at 900 MHz and an aperture width (the time the switch is on or pulse width)
`
`TON = 550 pico seconds = 550 ps. See Ex.-2007, 67:11-13. During the time the switch
`
`23
`
`
`
`is on, the energy available from the source = (62.5 nW) * (0.550 ns) = 34.38 * 10−18
`
`joules = 34.38 atto joules = 34.38 aJ.
`
`b.
`
`STEP 2: Energy stored on storage element.
`
`In the storage capacitance 8208 (i.e., storage element 8208) (denoted as C8208
`
`below), the charging time constant (when the switch is closed) is τPV,ON = (RS / RL)
`
`* C8208 = ((50 / 2000) ohms) * (18 pF) = (48.78 ohms) * (18 pF) = 878 pico seconds
`
`= 878 ps. The switch is on for TON = 550 ps and the ‘ON’ interval of the switch is
`
`centered on the 90 degree point as with Tayloe.19 The frequency of the input signal
`
`in the ParkerVision embodiment is 900 MHz, so the period of the input signal