# Micromagnetic Simulations of Hot-deformed Nd-Fe-B Magnets Subjected to Eutectic Grain Boundary Diffusion Process

https://mdr.nims.go.jp/datasets/e3d6e8c5-fa32-47b2-8d35-ebffa4919d9c

## File

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## Id

e3d6e8c5-fa32-47b2-8d35-ebffa4919d9c

## Local identifier



## Visibility

open_to_public

## State

published

## Created at

2025-08-15T02:55:30.350157Z

## Updated at

2025-08-20T03:31:18.130055Z

## Published at

2025-08-20T03:19:31.665943Z

## Doi

https://doi.org/10.48505/nims.5650

## First published url



## Date published



## Recorded date published



## Resource type

conference_presentation

## Manuscript type

na

## Collection

- id: d28f086a-61aa-4bc7-bcae-5a1078cbc6c7
  identifier: https://mdr.nims.go.jp/pid/d28f086a-61aa-4bc7-bcae-5a1078cbc6c7
  title: The 28th International Workshop on Rare Earth and Future Permanent Magnets
    and Their Applications (REPM2025)

## Title

- title: Micromagnetic Simulations of Hot-deformed Nd-Fe-B Magnets Subjected to Eutectic
    Grain Boundary Diffusion Process
  title_type: original
  lang: en

## Description

- description: "The grain boundary diffusion process (GBDP) using a low melting point
    alloy is recognized as an efficient technique for engineering the microstructure
    of hot-deformed Nd-Fe-B magnets aiming for high coercivity [1,2]. GBDP directly
    addresses the most critical microstructural feature affecting the coercivity that
    is a thin intergranular phase (IGP). This treatment is usually performed by coating
    a magnet with the eutectic alloy, e.g., Nd70Cu30, and then annealing at temperature
    500-600 °C. During this process, the Nd-rich liquid phase penetrates from the
    surface to the interior of the magnet through a network of triple junctions. At
    the same time, the liquid phase infiltrates between the grains, modifying the
    chemical composition of the IGP. Figure 1(a) shows a typical microstructure of
    a hot-deformed Nd-Fe-B magnet with an improved magnetic isolation of the Nd2Fe14B
    grains from each other after GBDP. This isolation is at the expense of the magnet’s
    remanence. Interestingly, while some grains are well separated by the thick Nd-rich
    phase, which is supposed to be nonmagnetic (Fig. 1b), other grains are still in
    contact through the thin magnetic IGP with Fe content similar to that in the IGP
    before GBDP (Fig. 1c). Thus, the grains are expected to be still exchange coupled,
    although the contact area for coupling tend to be decreased by GBDP. The question
    arises how the coercivity is influenced by the remaining exchange coupling and
    observed change of grain packing density, that apparently affects the magnetostatic
    interaction between grains. In this work, micromagnetic simulations were employed
    to address this question.\r\n\r\nTo imitate the microstructural transformations
    in hot-deformed Nd-Fe-B magnets after the Nd-based GBDP, a series of micromagnetic
    models was developed with a gradually increasing volume fraction of the nonmagnetic
    region, representing the infiltrated Nd-rich phase. One of these models is shown
    in Fig. 1d, demonstrating that there were also the regions of thin magnetic IGP
    which number and area decreased upon the GBDP. The mean grain size and aspect
    ratio were maintained constant. Micromagnetic simulations were used to analyze
    the tradeoff between coercivity and remanence as the magnetic properties of IGP
    (magnetization and exchange stiffness) and the volume fraction of Ndrich phase
    were varied systematically (Fig. 1e) [3]. These results allow to define realistic
    limits for coercivity achievable in hot-deformed Nd-Fe-B magnets via the Nd-based
    GBDP. The coercivity limits strongly depend on the IGP magnetization, which was
    estimated to be 0.9 ± 0.1 T by reproducing experimental Mr vs. Hc data from the
    literature. In this report, further extension of this study will be presented,
    accounting for the core-shell grain structure and covering other aspects of coercivity
    such as its angular and temperature dependencies.\r\n\r\nThe support by the MEXT
    (JPMXP1122715503) and JSPS (JP23H01674) is acknowledged.\r\n\r\nReferences\r\n[1]
    Hioki, Sci. Technol. Adv. Mater. 22 (2021) 72.\r\n[2] Sepehri-Amin et al., Acta
    Mater. 61 (2013) 6622.\r\n[3] Bolyachkin et al., Scripta Mater. 247 (2024) 116095."
  description_type: abstract
  lang: en

## Creator

- name: Anton Bolyachkin
  role: author
  organization: National Institute for Materials Science, Japan
- name: Xin Tang
  role: author
  organization: National Institute for Materials Science, Japan
- name: Nikita Kulesh
  role: author
  organization: National Institute for Materials Science, Japan
- name: Hossein Sepehri-Amin
  role: author
  organization: National Institute for Materials Science, Japan

## Contact agent



## Publisher

organization: National Institute for Materials Science (NIMS)

## Managing organization



## Keyword

- subject: REPM2025
  schema: not_defined
- subject: Micromagnetic simulations
  schema: not_defined
- subject: Nd-Fe-B magnets
  schema: not_defined
- subject: grain boundary diffusion
  schema: not_defined

## Rights

- identifier: https://creativecommons.org/licenses/by/4.0/

## Other identifier(s)



## Data origin

- data_origin_type: other

## Embargo



## Journal



## Conference

name: REPM2025
start_date: 2025-07-27
end_date: 2025-07-31
identifier: https://www.nims.go.jp/mmu/repm2025/

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## Fileset

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  filename: REPM2025_O14-2_Bolyachkin.pdf
  content_type: application/pdf
  size: 7076427
  md5: 47bfeca9573b351d6cf849bf636c0347
- id: 83ec6a83-2960-4179-b38e-427642ddec7e
  filename: "(abstract) O14-2_Figure1.jpeg"
  content_type: image/jpeg
  size: 68008
  md5: 55ee9f9946d9eb2971cc35b250bc0618

## Thumbnail

fileset_id: fc865ca8-b7f0-4d2b-9a26-57116464a9b0
filename: REPM2025_O14-2_Bolyachkin.pdf