Highly Efficient Metasurface Polarization Converter at Far-Infrared Range

Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversio...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Ahmed Mahfuz Tamim [verfasserIn] Md Mehedi Hasan [verfasserIn] Mohammad Rashed Iqbal Faruque [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2022

Schlagwörter:	metasurface polarization conversion terahertz x-polarized y-polarized

Übergeordnetes Werk:	In: Frontiers in Physics - Frontiers Media S.A., 2014, 10(2022)
Übergeordnetes Werk:	volume:10 ; year:2022

Links:	Link aufrufen Link aufrufen Link aufrufen Journal toc

DOI / URN:	10.3389/fphy.2022.890356

Katalog-ID:	DOAJ025907921

Internformat


LEADER	01000caa a22002652 4500
001	DOAJ025907921
003	DE-627
005	20230307093308.0
007	cr uuu---uuuuu
008	230226s2022 xx \|\|\|\|\|o 00\| \|\|eng c
024	7		\|a 10.3389/fphy.2022.890356 \|2 doi
035			\|a (DE-627)DOAJ025907921
035			\|a (DE-599)DOAJ34397760e1dc4aeaa2e33216b78f5cd2
040			\|a DE-627 \|b ger \|c DE-627 \|e rakwb
041			\|a eng
050		0	\|a QC1-999
100	0		\|a Ahmed Mahfuz Tamim \|e verfasserin \|4 aut
245	1	0	\|a Highly Efficient Metasurface Polarization Converter at Far-Infrared Range
264		1	\|c 2022
336			\|a Text \|b txt \|2 rdacontent
337			\|a Computermedien \|b c \|2 rdamedia
338			\|a Online-Ressource \|b cr \|2 rdacarrier
520			\|a Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversion using far-infrared frequency. Structural design, optimization, and results examination of the metasurface are performed using the CST microwave studio electromagnetic simulator. The metasurface was developed surrounding the two individual arrow-shaped metal resonators with two bar resonators on the opposite angular side of the arrow. Aluminum (Al) was used as a metallic resonator, while gallium arsenide (GaAs) was as the substrate. The interference theory was used to describe the co-polarized and cross-polarized reflectance coefficients, where two different mediums and interference layers were considered along with the reflected and transmitted wave. The polarization conversion efficiency yielded over 90% from 282.9 to 302.3 µm (0.987–1.062 THz) and 558.78 to 676.7 µm (0.442–0.537 THz) indicating multiple resonances at 286.7, 298.25, 586.1, and 689.55 µm. In conclusion, the performances and diverse characteristics of the designed metasurface demonstrated potential applications in the far-infrared spectrum as an efficient polarization converter application.
650		4	\|a metasurface
650		4	\|a polarization conversion
650		4	\|a terahertz
650		4	\|a x-polarized
650		4	\|a y-polarized
653		0	\|a Physics
700	0		\|a Md Mehedi Hasan \|e verfasserin \|4 aut
700	0		\|a Mohammad Rashed Iqbal Faruque \|e verfasserin \|4 aut
773	0	8	\|i In \|t Frontiers in Physics \|d Frontiers Media S.A., 2014 \|g 10(2022) \|w (DE-627)750371749 \|w (DE-600)2721033-9 \|x 2296424X \|7 nnns
773	1	8	\|g volume:10 \|g year:2022
856	4	0	\|u https://doi.org/10.3389/fphy.2022.890356 \|z kostenfrei
856	4	0	\|u https://doaj.org/article/34397760e1dc4aeaa2e33216b78f5cd2 \|z kostenfrei
856	4	0	\|u https://www.frontiersin.org/articles/10.3389/fphy.2022.890356/full \|z kostenfrei
856	4	2	\|u https://doaj.org/toc/2296-424X \|y Journal toc \|z kostenfrei
912			\|a GBV_USEFLAG_A
912			\|a SYSFLAG_A
912			\|a GBV_DOAJ
912			\|a GBV_ILN_11
912			\|a GBV_ILN_20
912			\|a GBV_ILN_22
912			\|a GBV_ILN_23
912			\|a GBV_ILN_24
912			\|a GBV_ILN_31
912			\|a GBV_ILN_39
912			\|a GBV_ILN_40
912			\|a GBV_ILN_60
912			\|a GBV_ILN_62
912			\|a GBV_ILN_63
912			\|a GBV_ILN_65
912			\|a GBV_ILN_69
912			\|a GBV_ILN_70
912			\|a GBV_ILN_73
912			\|a GBV_ILN_95
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_151
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_213
912			\|a GBV_ILN_230
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_2003
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_4012
912			\|a GBV_ILN_4037
912			\|a GBV_ILN_4112
912			\|a GBV_ILN_4125
912			\|a GBV_ILN_4126
912			\|a GBV_ILN_4249
912			\|a GBV_ILN_4305
912			\|a GBV_ILN_4306
912			\|a GBV_ILN_4307
912			\|a GBV_ILN_4313
912			\|a GBV_ILN_4322
912			\|a GBV_ILN_4323
912			\|a GBV_ILN_4324
912			\|a GBV_ILN_4325
912			\|a GBV_ILN_4335
912			\|a GBV_ILN_4338
912			\|a GBV_ILN_4367
912			\|a GBV_ILN_4700
951			\|a AR
952			\|d 10 \|j 2022

Indexfelder

author_variant	a m t amt m m h mmh m r i f mrif
matchkey_str	article:2296424X:2022----::ihyfiinmtsraeoaiainovrea
hierarchy_sort_str	2022
callnumber-subject-code	QC
publishDate	2022
allfields	10.3389/fphy.2022.890356 doi (DE-627)DOAJ025907921 (DE-599)DOAJ34397760e1dc4aeaa2e33216b78f5cd2 DE-627 ger DE-627 rakwb eng QC1-999 Ahmed Mahfuz Tamim verfasserin aut Highly Efficient Metasurface Polarization Converter at Far-Infrared Range 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversion using far-infrared frequency. Structural design, optimization, and results examination of the metasurface are performed using the CST microwave studio electromagnetic simulator. The metasurface was developed surrounding the two individual arrow-shaped metal resonators with two bar resonators on the opposite angular side of the arrow. Aluminum (Al) was used as a metallic resonator, while gallium arsenide (GaAs) was as the substrate. The interference theory was used to describe the co-polarized and cross-polarized reflectance coefficients, where two different mediums and interference layers were considered along with the reflected and transmitted wave. The polarization conversion efficiency yielded over 90% from 282.9 to 302.3 µm (0.987–1.062 THz) and 558.78 to 676.7 µm (0.442–0.537 THz) indicating multiple resonances at 286.7, 298.25, 586.1, and 689.55 µm. In conclusion, the performances and diverse characteristics of the designed metasurface demonstrated potential applications in the far-infrared spectrum as an efficient polarization converter application. metasurface polarization conversion terahertz x-polarized y-polarized Physics Md Mehedi Hasan verfasserin aut Mohammad Rashed Iqbal Faruque verfasserin aut In Frontiers in Physics Frontiers Media S.A., 2014 10(2022) (DE-627)750371749 (DE-600)2721033-9 2296424X nnns volume:10 year:2022 https://doi.org/10.3389/fphy.2022.890356 kostenfrei https://doaj.org/article/34397760e1dc4aeaa2e33216b78f5cd2 kostenfrei https://www.frontiersin.org/articles/10.3389/fphy.2022.890356/full kostenfrei https://doaj.org/toc/2296-424X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2003 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 10 2022
spelling	10.3389/fphy.2022.890356 doi (DE-627)DOAJ025907921 (DE-599)DOAJ34397760e1dc4aeaa2e33216b78f5cd2 DE-627 ger DE-627 rakwb eng QC1-999 Ahmed Mahfuz Tamim verfasserin aut Highly Efficient Metasurface Polarization Converter at Far-Infrared Range 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversion using far-infrared frequency. Structural design, optimization, and results examination of the metasurface are performed using the CST microwave studio electromagnetic simulator. The metasurface was developed surrounding the two individual arrow-shaped metal resonators with two bar resonators on the opposite angular side of the arrow. Aluminum (Al) was used as a metallic resonator, while gallium arsenide (GaAs) was as the substrate. The interference theory was used to describe the co-polarized and cross-polarized reflectance coefficients, where two different mediums and interference layers were considered along with the reflected and transmitted wave. The polarization conversion efficiency yielded over 90% from 282.9 to 302.3 µm (0.987–1.062 THz) and 558.78 to 676.7 µm (0.442–0.537 THz) indicating multiple resonances at 286.7, 298.25, 586.1, and 689.55 µm. In conclusion, the performances and diverse characteristics of the designed metasurface demonstrated potential applications in the far-infrared spectrum as an efficient polarization converter application. metasurface polarization conversion terahertz x-polarized y-polarized Physics Md Mehedi Hasan verfasserin aut Mohammad Rashed Iqbal Faruque verfasserin aut In Frontiers in Physics Frontiers Media S.A., 2014 10(2022) (DE-627)750371749 (DE-600)2721033-9 2296424X nnns volume:10 year:2022 https://doi.org/10.3389/fphy.2022.890356 kostenfrei https://doaj.org/article/34397760e1dc4aeaa2e33216b78f5cd2 kostenfrei https://www.frontiersin.org/articles/10.3389/fphy.2022.890356/full kostenfrei https://doaj.org/toc/2296-424X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2003 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 10 2022
allfields_unstemmed	10.3389/fphy.2022.890356 doi (DE-627)DOAJ025907921 (DE-599)DOAJ34397760e1dc4aeaa2e33216b78f5cd2 DE-627 ger DE-627 rakwb eng QC1-999 Ahmed Mahfuz Tamim verfasserin aut Highly Efficient Metasurface Polarization Converter at Far-Infrared Range 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversion using far-infrared frequency. Structural design, optimization, and results examination of the metasurface are performed using the CST microwave studio electromagnetic simulator. The metasurface was developed surrounding the two individual arrow-shaped metal resonators with two bar resonators on the opposite angular side of the arrow. Aluminum (Al) was used as a metallic resonator, while gallium arsenide (GaAs) was as the substrate. The interference theory was used to describe the co-polarized and cross-polarized reflectance coefficients, where two different mediums and interference layers were considered along with the reflected and transmitted wave. The polarization conversion efficiency yielded over 90% from 282.9 to 302.3 µm (0.987–1.062 THz) and 558.78 to 676.7 µm (0.442–0.537 THz) indicating multiple resonances at 286.7, 298.25, 586.1, and 689.55 µm. In conclusion, the performances and diverse characteristics of the designed metasurface demonstrated potential applications in the far-infrared spectrum as an efficient polarization converter application. metasurface polarization conversion terahertz x-polarized y-polarized Physics Md Mehedi Hasan verfasserin aut Mohammad Rashed Iqbal Faruque verfasserin aut In Frontiers in Physics Frontiers Media S.A., 2014 10(2022) (DE-627)750371749 (DE-600)2721033-9 2296424X nnns volume:10 year:2022 https://doi.org/10.3389/fphy.2022.890356 kostenfrei https://doaj.org/article/34397760e1dc4aeaa2e33216b78f5cd2 kostenfrei https://www.frontiersin.org/articles/10.3389/fphy.2022.890356/full kostenfrei https://doaj.org/toc/2296-424X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2003 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 10 2022
allfieldsGer	10.3389/fphy.2022.890356 doi (DE-627)DOAJ025907921 (DE-599)DOAJ34397760e1dc4aeaa2e33216b78f5cd2 DE-627 ger DE-627 rakwb eng QC1-999 Ahmed Mahfuz Tamim verfasserin aut Highly Efficient Metasurface Polarization Converter at Far-Infrared Range 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversion using far-infrared frequency. Structural design, optimization, and results examination of the metasurface are performed using the CST microwave studio electromagnetic simulator. The metasurface was developed surrounding the two individual arrow-shaped metal resonators with two bar resonators on the opposite angular side of the arrow. Aluminum (Al) was used as a metallic resonator, while gallium arsenide (GaAs) was as the substrate. The interference theory was used to describe the co-polarized and cross-polarized reflectance coefficients, where two different mediums and interference layers were considered along with the reflected and transmitted wave. The polarization conversion efficiency yielded over 90% from 282.9 to 302.3 µm (0.987–1.062 THz) and 558.78 to 676.7 µm (0.442–0.537 THz) indicating multiple resonances at 286.7, 298.25, 586.1, and 689.55 µm. In conclusion, the performances and diverse characteristics of the designed metasurface demonstrated potential applications in the far-infrared spectrum as an efficient polarization converter application. metasurface polarization conversion terahertz x-polarized y-polarized Physics Md Mehedi Hasan verfasserin aut Mohammad Rashed Iqbal Faruque verfasserin aut In Frontiers in Physics Frontiers Media S.A., 2014 10(2022) (DE-627)750371749 (DE-600)2721033-9 2296424X nnns volume:10 year:2022 https://doi.org/10.3389/fphy.2022.890356 kostenfrei https://doaj.org/article/34397760e1dc4aeaa2e33216b78f5cd2 kostenfrei https://www.frontiersin.org/articles/10.3389/fphy.2022.890356/full kostenfrei https://doaj.org/toc/2296-424X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2003 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 10 2022
allfieldsSound	10.3389/fphy.2022.890356 doi (DE-627)DOAJ025907921 (DE-599)DOAJ34397760e1dc4aeaa2e33216b78f5cd2 DE-627 ger DE-627 rakwb eng QC1-999 Ahmed Mahfuz Tamim verfasserin aut Highly Efficient Metasurface Polarization Converter at Far-Infrared Range 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversion using far-infrared frequency. Structural design, optimization, and results examination of the metasurface are performed using the CST microwave studio electromagnetic simulator. The metasurface was developed surrounding the two individual arrow-shaped metal resonators with two bar resonators on the opposite angular side of the arrow. Aluminum (Al) was used as a metallic resonator, while gallium arsenide (GaAs) was as the substrate. The interference theory was used to describe the co-polarized and cross-polarized reflectance coefficients, where two different mediums and interference layers were considered along with the reflected and transmitted wave. The polarization conversion efficiency yielded over 90% from 282.9 to 302.3 µm (0.987–1.062 THz) and 558.78 to 676.7 µm (0.442–0.537 THz) indicating multiple resonances at 286.7, 298.25, 586.1, and 689.55 µm. In conclusion, the performances and diverse characteristics of the designed metasurface demonstrated potential applications in the far-infrared spectrum as an efficient polarization converter application. metasurface polarization conversion terahertz x-polarized y-polarized Physics Md Mehedi Hasan verfasserin aut Mohammad Rashed Iqbal Faruque verfasserin aut In Frontiers in Physics Frontiers Media S.A., 2014 10(2022) (DE-627)750371749 (DE-600)2721033-9 2296424X nnns volume:10 year:2022 https://doi.org/10.3389/fphy.2022.890356 kostenfrei https://doaj.org/article/34397760e1dc4aeaa2e33216b78f5cd2 kostenfrei https://www.frontiersin.org/articles/10.3389/fphy.2022.890356/full kostenfrei https://doaj.org/toc/2296-424X Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2003 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 10 2022
language	English
source	In Frontiers in Physics 10(2022) volume:10 year:2022
sourceStr	In Frontiers in Physics 10(2022) volume:10 year:2022
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	metasurface polarization conversion terahertz x-polarized y-polarized Physics
isfreeaccess_bool	true
container_title	Frontiers in Physics
authorswithroles_txt_mv	Ahmed Mahfuz Tamim @@aut@@ Md Mehedi Hasan @@aut@@ Mohammad Rashed Iqbal Faruque @@aut@@
publishDateDaySort_date	2022-01-01T00:00:00Z
hierarchy_top_id	750371749
id	DOAJ025907921
language_de	englisch
fullrecord	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">DOAJ025907921</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230307093308.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230226s2022 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.3389/fphy.2022.890356</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)DOAJ025907921</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)DOAJ34397760e1dc4aeaa2e33216b78f5cd2</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="050" ind1=" " ind2="0"><subfield code="a">QC1-999</subfield></datafield><datafield tag="100" ind1="0" ind2=" "><subfield code="a">Ahmed Mahfuz Tamim</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Highly Efficient Metasurface Polarization Converter at Far-Infrared Range</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2022</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversion using far-infrared frequency. Structural design, optimization, and results examination of the metasurface are performed using the CST microwave studio electromagnetic simulator. The metasurface was developed surrounding the two individual arrow-shaped metal resonators with two bar resonators on the opposite angular side of the arrow. Aluminum (Al) was used as a metallic resonator, while gallium arsenide (GaAs) was as the substrate. The interference theory was used to describe the co-polarized and cross-polarized reflectance coefficients, where two different mediums and interference layers were considered along with the reflected and transmitted wave. The polarization conversion efficiency yielded over 90% from 282.9 to 302.3 µm (0.987–1.062 THz) and 558.78 to 676.7 µm (0.442–0.537 THz) indicating multiple resonances at 286.7, 298.25, 586.1, and 689.55 µm. In conclusion, the performances and diverse characteristics of the designed metasurface demonstrated potential applications in the far-infrared spectrum as an efficient polarization converter application.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">metasurface</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">polarization conversion</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">terahertz</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">x-polarized</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">y-polarized</subfield></datafield><datafield tag="653" ind1=" " ind2="0"><subfield code="a">Physics</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Md Mehedi Hasan</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Mohammad Rashed Iqbal Faruque</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">In</subfield><subfield code="t">Frontiers in Physics</subfield><subfield code="d">Frontiers Media S.A., 2014</subfield><subfield code="g">10(2022)</subfield><subfield code="w">(DE-627)750371749</subfield><subfield code="w">(DE-600)2721033-9</subfield><subfield code="x">2296424X</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:10</subfield><subfield code="g">year:2022</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doi.org/10.3389/fphy.2022.890356</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doaj.org/article/34397760e1dc4aeaa2e33216b78f5cd2</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://www.frontiersin.org/articles/10.3389/fphy.2022.890356/full</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://doaj.org/toc/2296-424X</subfield><subfield code="y">Journal toc</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_DOAJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2003</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4367</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">10</subfield><subfield code="j">2022</subfield></datafield></record></collection>
callnumber-first	Q - Science
author	Ahmed Mahfuz Tamim
spellingShingle	Ahmed Mahfuz Tamim misc QC1-999 misc metasurface misc polarization conversion misc terahertz misc x-polarized misc y-polarized misc Physics Highly Efficient Metasurface Polarization Converter at Far-Infrared Range
authorStr	Ahmed Mahfuz Tamim
ppnlink_with_tag_str_mv	@@773@@(DE-627)750371749
format	electronic Article
delete_txt_mv	keep
author_role	aut aut aut
collection	DOAJ
remote_str	true
callnumber-label	QC1-999
illustrated	Not Illustrated
issn	2296424X
topic_title	QC1-999 Highly Efficient Metasurface Polarization Converter at Far-Infrared Range metasurface polarization conversion terahertz x-polarized y-polarized
topic	misc QC1-999 misc metasurface misc polarization conversion misc terahertz misc x-polarized misc y-polarized misc Physics
topic_unstemmed	misc QC1-999 misc metasurface misc polarization conversion misc terahertz misc x-polarized misc y-polarized misc Physics
topic_browse	misc QC1-999 misc metasurface misc polarization conversion misc terahertz misc x-polarized misc y-polarized misc Physics
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
format_main_str_mv	Text Zeitschrift/Artikel
carriertype_str_mv	cr
hierarchy_parent_title	Frontiers in Physics
hierarchy_parent_id	750371749
hierarchy_top_title	Frontiers in Physics
isfreeaccess_txt	true
familylinks_str_mv	(DE-627)750371749 (DE-600)2721033-9
title	Highly Efficient Metasurface Polarization Converter at Far-Infrared Range
ctrlnum	(DE-627)DOAJ025907921 (DE-599)DOAJ34397760e1dc4aeaa2e33216b78f5cd2
title_full	Highly Efficient Metasurface Polarization Converter at Far-Infrared Range
author_sort	Ahmed Mahfuz Tamim
journal	Frontiers in Physics
journalStr	Frontiers in Physics
callnumber-first-code	Q
lang_code	eng
isOA_bool	true
recordtype	marc
publishDateSort	2022
contenttype_str_mv	txt
author_browse	Ahmed Mahfuz Tamim Md Mehedi Hasan Mohammad Rashed Iqbal Faruque
container_volume	10
class	QC1-999
format_se	Elektronische Aufsätze
author-letter	Ahmed Mahfuz Tamim
doi_str_mv	10.3389/fphy.2022.890356
author2-role	verfasserin
title_sort	highly efficient metasurface polarization converter at far-infrared range
callnumber	QC1-999
title_auth	Highly Efficient Metasurface Polarization Converter at Far-Infrared Range
abstract	Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversion using far-infrared frequency. Structural design, optimization, and results examination of the metasurface are performed using the CST microwave studio electromagnetic simulator. The metasurface was developed surrounding the two individual arrow-shaped metal resonators with two bar resonators on the opposite angular side of the arrow. Aluminum (Al) was used as a metallic resonator, while gallium arsenide (GaAs) was as the substrate. The interference theory was used to describe the co-polarized and cross-polarized reflectance coefficients, where two different mediums and interference layers were considered along with the reflected and transmitted wave. The polarization conversion efficiency yielded over 90% from 282.9 to 302.3 µm (0.987–1.062 THz) and 558.78 to 676.7 µm (0.442–0.537 THz) indicating multiple resonances at 286.7, 298.25, 586.1, and 689.55 µm. In conclusion, the performances and diverse characteristics of the designed metasurface demonstrated potential applications in the far-infrared spectrum as an efficient polarization converter application.
abstractGer	Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversion using far-infrared frequency. Structural design, optimization, and results examination of the metasurface are performed using the CST microwave studio electromagnetic simulator. The metasurface was developed surrounding the two individual arrow-shaped metal resonators with two bar resonators on the opposite angular side of the arrow. Aluminum (Al) was used as a metallic resonator, while gallium arsenide (GaAs) was as the substrate. The interference theory was used to describe the co-polarized and cross-polarized reflectance coefficients, where two different mediums and interference layers were considered along with the reflected and transmitted wave. The polarization conversion efficiency yielded over 90% from 282.9 to 302.3 µm (0.987–1.062 THz) and 558.78 to 676.7 µm (0.442–0.537 THz) indicating multiple resonances at 286.7, 298.25, 586.1, and 689.55 µm. In conclusion, the performances and diverse characteristics of the designed metasurface demonstrated potential applications in the far-infrared spectrum as an efficient polarization converter application.
abstract_unstemmed	Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversion using far-infrared frequency. Structural design, optimization, and results examination of the metasurface are performed using the CST microwave studio electromagnetic simulator. The metasurface was developed surrounding the two individual arrow-shaped metal resonators with two bar resonators on the opposite angular side of the arrow. Aluminum (Al) was used as a metallic resonator, while gallium arsenide (GaAs) was as the substrate. The interference theory was used to describe the co-polarized and cross-polarized reflectance coefficients, where two different mediums and interference layers were considered along with the reflected and transmitted wave. The polarization conversion efficiency yielded over 90% from 282.9 to 302.3 µm (0.987–1.062 THz) and 558.78 to 676.7 µm (0.442–0.537 THz) indicating multiple resonances at 286.7, 298.25, 586.1, and 689.55 µm. In conclusion, the performances and diverse characteristics of the designed metasurface demonstrated potential applications in the far-infrared spectrum as an efficient polarization converter application.
collection_details	GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2003 GBV_ILN_2014 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700
title_short	Highly Efficient Metasurface Polarization Converter at Far-Infrared Range
url	https://doi.org/10.3389/fphy.2022.890356 https://doaj.org/article/34397760e1dc4aeaa2e33216b78f5cd2 https://www.frontiersin.org/articles/10.3389/fphy.2022.890356/full https://doaj.org/toc/2296-424X
remote_bool	true
author2	Md Mehedi Hasan Mohammad Rashed Iqbal Faruque
author2Str	Md Mehedi Hasan Mohammad Rashed Iqbal Faruque
ppnlink	750371749
callnumber-subject	QC - Physics
mediatype_str_mv	c
isOA_txt	true
hochschulschrift_bool	false
doi_str	10.3389/fphy.2022.890356
callnumber-a	QC1-999
up_date	2024-07-03T17:52:46.678Z
_version_	1803581303477501952
fullrecord_marcxml	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">DOAJ025907921</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230307093308.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230226s2022 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.3389/fphy.2022.890356</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)DOAJ025907921</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)DOAJ34397760e1dc4aeaa2e33216b78f5cd2</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="050" ind1=" " ind2="0"><subfield code="a">QC1-999</subfield></datafield><datafield tag="100" ind1="0" ind2=" "><subfield code="a">Ahmed Mahfuz Tamim</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Highly Efficient Metasurface Polarization Converter at Far-Infrared Range</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2022</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Controlling the polarization state is an efficient way to enhance the functionalities in sensing, imaging, and communication systems in the microwave and terahertz (THz) spectrum. This study proposed an anisotropic metasurface and numerically explained it as a highly efficient polarization conversion using far-infrared frequency. Structural design, optimization, and results examination of the metasurface are performed using the CST microwave studio electromagnetic simulator. The metasurface was developed surrounding the two individual arrow-shaped metal resonators with two bar resonators on the opposite angular side of the arrow. Aluminum (Al) was used as a metallic resonator, while gallium arsenide (GaAs) was as the substrate. The interference theory was used to describe the co-polarized and cross-polarized reflectance coefficients, where two different mediums and interference layers were considered along with the reflected and transmitted wave. The polarization conversion efficiency yielded over 90% from 282.9 to 302.3 µm (0.987–1.062 THz) and 558.78 to 676.7 µm (0.442–0.537 THz) indicating multiple resonances at 286.7, 298.25, 586.1, and 689.55 µm. In conclusion, the performances and diverse characteristics of the designed metasurface demonstrated potential applications in the far-infrared spectrum as an efficient polarization converter application.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">metasurface</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">polarization conversion</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">terahertz</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">x-polarized</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">y-polarized</subfield></datafield><datafield tag="653" ind1=" " ind2="0"><subfield code="a">Physics</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Md Mehedi Hasan</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Mohammad Rashed Iqbal Faruque</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">In</subfield><subfield code="t">Frontiers in Physics</subfield><subfield code="d">Frontiers Media S.A., 2014</subfield><subfield code="g">10(2022)</subfield><subfield code="w">(DE-627)750371749</subfield><subfield code="w">(DE-600)2721033-9</subfield><subfield code="x">2296424X</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:10</subfield><subfield code="g">year:2022</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doi.org/10.3389/fphy.2022.890356</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doaj.org/article/34397760e1dc4aeaa2e33216b78f5cd2</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://www.frontiersin.org/articles/10.3389/fphy.2022.890356/full</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://doaj.org/toc/2296-424X</subfield><subfield code="y">Journal toc</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_DOAJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_63</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_65</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_151</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_213</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_230</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2003</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4037</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4112</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4125</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4249</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4305</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4306</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4307</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4322</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4324</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4325</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4335</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4338</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4367</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">10</subfield><subfield code="j">2022</subfield></datafield></record></collection>
score	7.3985004

Nicht das Richtige dabei?

Schreiben Sie uns!

Highly Efficient Metasurface Polarization Converter at Far-Infrared Range

Nicht das Richtige dabei?

Zugang & Verfügbarkeit

Vorhandene Bände

Nicht das Richtige dabei?