Lambeth Magnetic Structures, LLC v. Seagate Technology (Us) Holdings Inc.

Court of Appeals for the Federal Circuit·Decided September 17, 2025·No. 23-1335·Unpublished

Opinion

NOTE: This disposition is nonprecedential.

United States Court of Appeals for the Federal Circuit

LAMBETH MAGNETIC STRUCTURES, LLC, Plaintiff-Appellant

v.

SEAGATE TECHNOLOGY (US) HOLDINGS INC., SEAGATE TECHNOLOGY, LLC, Defendants-Cross-Appellants

2023-1335, 2023-1346

Appeals from the United States District Court for the Western District of Pennsylvania in No. 2:16-cv-00538-CB, Judge Cathy Bissoon.

Decided: September 17, 2025

JEFFREY A. LAMKEN, MoloLamken LLP, Washington, DC, argued for plaintiff-appellant. Also represented by JENNIFER ELIZABETH FISCHELL, RAYINER HASHEM; DENISE MARIE DE MORY, MICHAEL ELI FLYNN-O'BRIEN, RICHARD CHENG-HONG LIN, Bunsow De Mory LLP, Redwood City, CA.

DAVID J.F. GROSS, Faegre Drinker Biddle & Reath LLP, Minneapolis, MN, argued for defendants-cross-appellants.

2 LAMBETH MAGNETIC STRUCTURES, LLC v.

SEAGATE TECHNOLOGY (US) HOLDINGS INC.

Also represented by CHAD DROWN, KATHERINE S. RAZAVI, KEVIN P. WAGNER.

Before REYNA, SCHALL, and HUGHES, Circuit Judges.

REYNA, Circuit Judge.

Lambeth Magnetic Structures, LLC appeals a district court judgment of noninfringement of its U.S. Patent No. 7,128,988. Lambeth argues that the district court erroneously construed the claim term “uniaxial symmetry broken structure.” Seagate Technology (US) Holdings Inc. and Seagate Technology, LLC cross-appeal, arguing that the district court erred in denying judgment as a matter of law on invalidity, because a reasonable jury could not have found the patent enabled under 35 U.S.C. § 112. We determine that the district court’s judgment of noninfringement was premised on an erroneous claim construction of the disputed claim term. We vacate the judgment of noninfringement and dismiss the cross-appeal as improper. Because we determine that the proper construction of the disputed claim term may affect the evidence and arguments presented on enablement, we remand for a new trial on both infringement and enablement under the proper construction of “uniaxial symmetry broken structure.”

BACKGROUND

I. The ’988 Patent

Dr. David N. Lambeth (“Dr. Lambeth”) originally assigned U.S. Patent No. 7,128,988 (“’988 patent”) to Lambeth Systems. ’988 patent; see also J.A. 30234. That patent is currently assigned to Lambeth Magnetic Structures , LLC (“LMS”). J.A. 12585. The patent relates to “[a] thin film magnetic structure, magnetic devices, and method of producing the same.” Id., Abstract. One use case for the invention is in “magnetic recording media” devices , id. at 6:65–7:3, 32:33–34, such as hard disk drives

LAMBETH MAGNETIC STRUCTURES, LLC v. 3 SEAGATE TECHNOLOGY (US) HOLDINGS INC.

(“hard drives”). See J.A. 24. In “a traditional hard disk system,” a “magnetic head passes over the media data,” i.e., the hard disk. ’988 patent, 7:12–16, 35–56. To record information on the disk, the magnetic head can apply a magnetic field that alters the media data, see id. at 7:35–38; in this case, the head is referred to as a “recording head,” see id. at 7:12–20. The patent is directed to a particular “thin film” magnetic material that can be used in such recording heads. Id. at 12:58–66.

The patent describes what it purports to be a unique structure for such a thin-film material. See id. at 12:58–13:18. Specifically, the patent describes the structure as including three features relevant to this appeal . The first feature is that the structure includes “at least one bcc-d layer which is magnetic.” Id. at claim 1. A “bcc-d layer” is a layer of metallic crystals in which the metal atoms are arranged in a “body centered cubic” or a derivative thereof (“bcc-d” or “bcc’d”) manner; thus, “bcc” refers to a type of crystal structure. Id. at 5:12–17, 14:64–67; see J.A. 24325. The patent provides that using a bcc-d layer increases “saturation magnetization[]” in comparison to layers consisting of other types of crystal structures , thereby “allow[ing] new devices to be constructed” with favorable properties such as “high magnetization.” Id. at 13:2–8. According to Dr. Lambeth, for “magnetic recording heads,” high magnetization allows the head to “put out a stronger field towards the media.” J.A. 30138–39.

The second feature is that the bcc-d layer “form[s] a uniaxial symmetry broken structure.” ’988 patent, claim 1. “Uniaxial” as used in the patent refers to “uniaxial anisotropy .” See id. at 1:45–60 (defining “uniaxial anisotropy”), 3:11–27 (referring to materials demonstrating uniaxial anisotropy as “uniaxial materials”). “Magnetic anisotropy” (or simply “anisotropy”) occurs when a material can be more easily magnetized in a particular direction. Id. at 1:35–60. That is, the material has a “preferred direction, or directions, of [magnetic] orientation.” Id. at 1:35–38. An 4 LAMBETH MAGNETIC STRUCTURES, LLC v.

SEAGATE TECHNOLOGY (US) HOLDINGS INC.

anisotropic material is uniaxial when it has a single direction , the “easy axis,” along which magnetization is preferred , and a single different direction, the “hard axis,” along which magnetization is not preferred, as the magnetization angle is rotated by 180 degrees from a physical axis. Id. at 1:35–60. In the context of a recording head, the patent explains that using a material that is uniaxially anisotropic allows the head to be magnetized to turn away from the media, i.e., the hard disk, after recording on it, to avoid “generat[ing] noise” that may inadvertently overwrite nearby areas of the media. Id. at 7:32–67. Dr. Lambeth testified that he aimed to create a head with properties such that, after recording on the media, the head “turns back, so it doesn’t erase the media.” J.A. 30143.

The third relevant feature required by the claims is that the structure is “symmetry broken.” ’988 patent, claim 1. A symmetry-broken structure refers to a subset of possible arrangements of the bcc-d “unit cells,” which comprise the crystal lattice that makes up the structure. Id. at 11:33–49, 16:34–36. The bcc-d unit cells in the claimed structure can be oriented in one of six directions or “variants ” over a hexagonal template. Id. at 13:39–42, 14:48–58. A “symmetry broken structure” occurs when the material does “not contain an equal amount of all six of” the “bcc-d variants.” Id. at 23:38–41. According to the patent , “uniaxial behavior can result” from symmetry broken structure. Id. at 23:50–24:8 (emphasis added).

On appeal, the claims at issue are claims 1, 3, 6, 7, 9, 17, 19, and 27–29 of the ’988 patent. Independent claim 1 is representative:

1. A magnetic material structure comprising: a substrate; at least one bcc-d layer which is magnetic, forming a uniaxial symmetry broken structure; and

LAMBETH MAGNETIC STRUCTURES, LLC v. 5 SEAGATE TECHNOLOGY (US) HOLDINGS INC.

at least one layer providing a . . . textured hexagonal atomic template disposed between said substrate and said bcc-d layer.

Id. at claim 1 (emphasis added).

II. Procedural History

In 2016, LMS sued several hard drive manufacturers, including Seagate Technology (US) Holdings Inc. and Seagate Technology, LLC (collectively, “Seagate”), in the United States District Court for the Western District of Pennsylvania, alleging infringement of the ’988 patent.1 In the complaint, LMS alleged that Seagate’s products “infringe at least claims 1 and 27 of the ’988 patent, and dependent claims thereof, including claims 6, 7, 9, 11, and 13.” J.A. 201.

In October 2017, the district court issued a Markman order. J.A. 1–21. The district court construed the claim term “uniaxial symmetry broken structure” as “a structure that is uniaxial as a result of the structure being symmetry broken.” J.A. 18–20 (emphasis added).

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