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Saha S, Acharya S, Popov M, Sauyet T, Pfund J, Bidthanapally R, Jain M, Page MR, Srinivasan G. A Novel Spinel Ferrite-Hexagonal Ferrite Composite for Enhanced Magneto-Electric Coupling in a Bilayer with PZT. Sensors (Basel) 2023; 23:9815. [PMID: 38139661 PMCID: PMC10748018 DOI: 10.3390/s23249815] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/17/2023] [Revised: 12/06/2023] [Accepted: 12/11/2023] [Indexed: 12/24/2023]
Abstract
The magnetoelectric effect (ME) is an important strain mediated-phenomenon in a ferromagnetic-piezoelectric composite for a variety of sensors and signal processing devices. A bias magnetic field, in general, is essential to realize a strong ME coupling in most composites. Magnetic phases with (i) high magnetostriction for strong piezomagnetic coupling and (ii) large anisotropy field that acts as a built-in bias field are preferred so that miniature, ME composite-based devices can operate without the need for an external magnetic field. We are able to realize such a magnetic phase with a composite of (i) barium hexaferrite (BaM) with high magnetocrystalline anisotropy field and (ii) nickel ferrite (NFO) with high magnetostriction. The BNx composites, with (100 - x) wt.% of BaM and x wt.% NFO, for x = 0-100, were prepared. X-ray diffraction analysis shows that the composites did not contain any impurity phases. Scanning electron microscopy images revealed that, with an increase in NFO content, hexagonal BaM grains become prominent, leading to a large anisotropy field. The room temperature saturation magnetization showed a general increase with increasing BaM content in the composites. NFO rich composites with x ≥ 60 were found to have a large magnetostriction value of around -23 ppm, comparable to pure NFO. The anisotropy field HA of the composites, determined from magnetization and ferromagnetic resonance (FMR) measurements, increased with increasing NFO content and reached a maximum of 7.77 kOe for x = 75. The BNx composite was cut into rectangular platelets and bonded with PZT to form the bilayers. ME voltage coefficient (MEVC) measurements at low frequencies and at mechanical resonance showed strong coupling at zero bias for samples with x ≥ 33. This large in-plane HA acted as a built-in field for strong ME effects under zero external bias in the bilayers. The highest zero-bias MEVC of ~22 mV/cm Oe was obtained for BN75-PZT bilayers wherein BN75 also has the highest HA. The Bilayer of BN95-PZT showed a maximum MEVC ~992 mV/cm Oe at electromechanical resonance at 59 kHz. The use of hexaferrite-spinel ferrite composite to achieve strong zero-bias ME coupling in bilayers with PZT is significant for applications related to energy harvesting, sensors, and high frequency devices.
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Affiliation(s)
- Sujoy Saha
- Department of Physics, Oakland University, Rochester, MI 48309, USA; (S.S.); (S.A.); (M.P.); (R.B.)
| | - Sabita Acharya
- Department of Physics, Oakland University, Rochester, MI 48309, USA; (S.S.); (S.A.); (M.P.); (R.B.)
| | - Maksym Popov
- Department of Physics, Oakland University, Rochester, MI 48309, USA; (S.S.); (S.A.); (M.P.); (R.B.)
- Institute of High Technologies, Taras Shevchenko National University of Kyiv, 01601 Kyiv, Ukraine
| | - Theodore Sauyet
- Department of Physics, University of Connecticut, Storrs, CT 06269, USA; (T.S.); (J.P.); (M.J.)
| | - Jacob Pfund
- Department of Physics, University of Connecticut, Storrs, CT 06269, USA; (T.S.); (J.P.); (M.J.)
| | - Rao Bidthanapally
- Department of Physics, Oakland University, Rochester, MI 48309, USA; (S.S.); (S.A.); (M.P.); (R.B.)
| | - Menka Jain
- Department of Physics, University of Connecticut, Storrs, CT 06269, USA; (T.S.); (J.P.); (M.J.)
| | - Michael R. Page
- Materials and Manufacturing Directorate, Air Force Research Laboratory, Wright-Patterson Air Force Base, Dayton, OH 45433, USA;
| | - Gopalan Srinivasan
- Department of Physics, Oakland University, Rochester, MI 48309, USA; (S.S.); (S.A.); (M.P.); (R.B.)
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Chorsi MT, Le TT, Lin F, Vinikoor T, Das R, Stevens JF, Mundrane C, Park J, Tran KT, Liu Y, Pfund J, Thompson R, He W, Jain M, Morales-Acosta MD, Bilal OR, Kazerounian K, Ilies H, Nguyen TD. Highly piezoelectric, biodegradable, and flexible amino acid nanofibers for medical applications. Sci Adv 2023; 9:eadg6075. [PMID: 37315129 PMCID: PMC10266740 DOI: 10.1126/sciadv.adg6075] [Citation(s) in RCA: 8] [Impact Index Per Article: 8.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/10/2023] [Accepted: 05/10/2023] [Indexed: 06/16/2023]
Abstract
Amino acid crystals are an attractive piezoelectric material as they have an ultrahigh piezoelectric coefficient and have an appealing safety profile for medical implant applications. Unfortunately, solvent-cast films made from glycine crystals are brittle, quickly dissolve in body fluid, and lack crystal orientation control, reducing the overall piezoelectric effect. Here, we present a material processing strategy to create biodegradable, flexible, and piezoelectric nanofibers of glycine crystals embedded inside polycaprolactone (PCL). The glycine-PCL nanofiber film exhibits stable piezoelectric performance with a high ultrasound output of 334 kPa [under 0.15 voltage root-mean-square (Vrms)], which outperforms the state-of-the-art biodegradable transducers. We use this material to fabricate a biodegradable ultrasound transducer for facilitating the delivery of chemotherapeutic drug to the brain. The device remarkably enhances the animal survival time (twofold) in mice-bearing orthotopic glioblastoma models. The piezoelectric glycine-PCL presented here could offer an excellent platform not only for glioblastoma therapy but also for developing medical implantation fields.
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Affiliation(s)
- Meysam T. Chorsi
- Department of Mechanical Engineering, University of Connecticut, Storrs, CT 06269, USA
- Department of Biomedical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Thinh T. Le
- Department of Mechanical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Feng Lin
- Department of Mechanical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Tra Vinikoor
- Department of Biomedical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Ritopa Das
- Department of Biomedical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - James F. Stevens
- Department of Mechanical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Caitlyn Mundrane
- Department of Biomedical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Jinyoung Park
- Department of Biomedical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Khanh T. M. Tran
- Department of Biomedical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Yang Liu
- Department of Mechanical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Jacob Pfund
- Department of Physics, University of Connecticut, Storrs, CT 06269, USA
| | - Rachel Thompson
- Department of Biomedical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Wu He
- Flow Cytometry Facility, Center for Open Research Resources and Equipment, University of Connecticut, Storrs, CT 06269, USA
| | - Menka Jain
- Department of Physics, University of Connecticut, Storrs, CT 06269, USA
- Institute of Materials Science, University of Connecticut, Storrs, CT 06269, USA
| | | | - Osama R. Bilal
- Department of Mechanical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Kazem Kazerounian
- Department of Mechanical Engineering, University of Connecticut, Storrs, CT 06269, USA
- Department of Biomedical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Horea Ilies
- Department of Mechanical Engineering, University of Connecticut, Storrs, CT 06269, USA
| | - Thanh D. Nguyen
- Department of Mechanical Engineering, University of Connecticut, Storrs, CT 06269, USA
- Department of Biomedical Engineering, University of Connecticut, Storrs, CT 06269, USA
- Institute of Materials Science, University of Connecticut, Storrs, CT 06269, USA
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Abstract
An optical setup for the testing of rotationally symmetric aspheres without a null optic is proposed. The optical setup is able to transfer the strongly curved wave fronts that stem from the reflection of a spherical testing wave front at a rotationally symmetric asphere. By simulation it is proved that the algorithms of the Shack-Hartmann sensor that is used can cope with the steep wave-front slopes (approximately 110lambda/mm) in the detection plane. The systematic errors of the testing configuration are analyzed and separated. For all types of error, functionals are derived whose significance is proved by simulation. The maximum residual errors in the simulations are fewer than lambda/500 (peak to valley).
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Affiliation(s)
- J Pfund
- Lehrstuhl für Optik, Universität Erlangen-Nürnberg, Staudtstrasse 7, D-91058 Erlangen, Germany.
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Groening S, Sick B, Donner K, Pfund J, Lindlein N, Schwider J. Wave-front reconstruction with a shack-hartmann sensor with an iterative spline fitting method. Appl Opt 2000; 39:561-567. [PMID: 18337926 DOI: 10.1364/ao.39.000561] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/26/2023]
Abstract
One limitation of the conventional Shack-Hartmann sensor is that the spots of each microlens have to remain in their respective subapertures. We present an algorithm that assigns the spots to their reference points unequivocally even if they are situated far outside their subaperture. For this assignment a spline function is extrapolated in successive steps of the iterative algorithm. The proposed method works in a single-shot technique and does not need any aid from mechanical devices. The reconstruction of a simulated steep aspherical wave front (approximately 100 lambda/mm slope) is described as well as experimental results of the measurement of a spherical wave front with a huge peak-to-valley value (approximately 400 lambda). The performance of the method is compared with the unwrapping method, which has been published before.
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Affiliation(s)
- S Groening
- Donner are with FORWISS, Universität Passau, Innstrasse 33, D-94032 Passau, Germany.
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Pfund J, Lindlein N, Schwider J. Dynamic range expansion of a Shack-Hartmann sensor by use of a modified unwrapping algorithm. Opt Lett 1998; 23:995-997. [PMID: 18087407 DOI: 10.1364/ol.23.000995] [Citation(s) in RCA: 11] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/25/2023]
Abstract
An algorithm for expanding the dynamic range of Shack--Hartmann sensors is proposed. The distribution of the spot dislocations is treated with a modified unwrapping algorithm that is widely used in interferometry. The algorithm unwraps the spot dislocations and assigns the spots to their original subapertures, leading to a huge expansion of the dynamic range. For the proposed algorithm there remains a limitation on the maximum wave-front curvature instead of on the maximum wave-front slope. Examples are given that show spot fields that were wrapped four times; the measured wave front had a peak-to-valley value of 116 lambda .
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Affiliation(s)
- J Pfund
- Physikalisches Institut der Universität Erlangen-Nürnberg, Staudtstrasse 7, 91058 Erlangen, Germany
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Pfund J, Lindlein N, Schwider J, Burow R, Blümel T, Elssner KE. Absolute sphericity measurement: a comparative study of the use of interferometry and a Shack-Hartmann sensor. Opt Lett 1998; 23:742-744. [PMID: 18087327 DOI: 10.1364/ol.23.000742] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/25/2023]
Abstract
A comparison of absolute sphericity measurements with a ShackHartmann sensor and a TwymanGreen interferometer is presented. The absolute deviations of a test sphere from its ideal shape were calculated in both cases from the measured wave aberrations of three different positions. Very good qualitative and quantitative agreement of the results was achieved. The difference of the root-mean-square values of the two methods was 1/1000 of a wavelength.
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Werner BL, Cho PS, Pfund J. The FE-lspd model for electron beam dosimetry. Phys Med Biol 1998; 43:291-311. [PMID: 9509527 DOI: 10.1088/0031-9155/43/2/006] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/06/2023]
Abstract
The FE-lspd model is a two-component electron beam model that distinguishes between electrons that can be described by small-angle transport theory and electrons that are too widely scattered for small-angle transport theory to be applicable. The two components are called the primary beam and the laterally scattered primary distribution (lspd). The primary beam component incorporates a simple version of the Fermi-Eyges model and dominates dose calculations at therapeutic depths. The lspd component corrects erros in the lateral spreading of the primary beam component, thereby improving the accuracy by which the FE-lspd model calculates dose distribution in blocked fields. Comparisons were made between dose profiles and central-axis depth dose distributions in small fields calculated by the FE-lspd, Fermi-Eyges and EGS4 Monte Carlo models for a 10 MeV beam in a homogeneous water phantom. The maximum difference between the dose calculated using the FE-lspd model and EGS4 Monte Carlo is about 6% at a field diameter of about 1 cm, and less than 2% for field sizes greater than 3 cm diameter. The maximum difference between the Fermi-Eyges and Monte Carlo calculations is about 18% at a field diameter of about 2.5 cm. A comparison was made with the central-axis depth dose distribution measured in water for a 3 cm diameter field in a 10 MeV clinical electron beam. The errors in the dose distribution were found to be less than 2% using the FE-lspd model but almost 18% using the Fermi-Eyges model. A comparison was also made with pencil beam profiles calculated using the second-order Fermi-Eyges transport model.
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Affiliation(s)
- B L Werner
- Oncology Systems, Picker International, Inc., Wayne, PA 19087, USA
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Abstract
The Shack-Hartmann sensor uses a microlens array and a CCD camera for wave-front measurements. To obtain wave-front measurements with high accuracy, an accurate relative alignment of both is essential. The different states of misalignment of the Shack-Hartmann sensor are divided into groups and are treated theoretically and experimentally. Their effect on the accuracy of wave-front measurements is evaluated. In addition, a practical method for proper alignment of the Shack-Hartmann sensor is proposed.
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Affiliation(s)
- J Pfund
- Lehrstuhl für Optik, Universität Erlangen-Nürnberg, Physikalisches Institut, D-91058 Erlangen, Staudtstrasse 7/B2, Germany
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