Electric field induced gap modification in ultrathin blue phosphorus
We investigate the possibility of band structure engineering in the recently predicted 2D layered form of blue phosphorus via an electric field (E sub(z)) applied perpendicular to the layer(s). Using density functional theory, we study the effect of a transverse electric field in monolayer as well a...
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Veröffentlicht in: | Physical review. B, Condensed matter and materials physics Condensed matter and materials physics, 2015-03, Vol.91 (11), Article 115433 |
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creator | Ghosh, Barun Nahas, Suhas Bhowmick, Somnath Agarwal, Amit |
description | We investigate the possibility of band structure engineering in the recently predicted 2D layered form of blue phosphorus via an electric field (E sub(z)) applied perpendicular to the layer(s). Using density functional theory, we study the effect of a transverse electric field in monolayer as well as three differently stacked bilayer structures of blue phosphorus. We find that for E sub(z) > 0.2 V/[Angstrom] the direct energy gap at the [Gamma] point, which is much larger than the default indirect band gap of mono- and bilayer blue phosphorus, decreases linearly with the increasing electric field, becomes comparable to the default indirect band gap at E sub(z) [asymptotically =] 0.45 (0.35) V/[Angstrom] for monolayer (bilayers), and decreases further until the semiconductor to metal transition of 2D blue phosphorus takes place at E sub(z) [asymptotically =] 0.7 (0.5) V/[Angstrom] for monolayer (bilayers). Calculated values of the electron and hole effective masses along various high symmetry directions in the reciprocal lattice suggests that the mobility of charge carriers is also influenced by the applied electric field. |
doi_str_mv | 10.1103/PhysRevB.91.115433 |
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Using density functional theory, we study the effect of a transverse electric field in monolayer as well as three differently stacked bilayer structures of blue phosphorus. We find that for E sub(z) > 0.2 V/[Angstrom] the direct energy gap at the [Gamma] point, which is much larger than the default indirect band gap of mono- and bilayer blue phosphorus, decreases linearly with the increasing electric field, becomes comparable to the default indirect band gap at E sub(z) [asymptotically =] 0.45 (0.35) V/[Angstrom] for monolayer (bilayers), and decreases further until the semiconductor to metal transition of 2D blue phosphorus takes place at E sub(z) [asymptotically =] 0.7 (0.5) V/[Angstrom] for monolayer (bilayers). 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B, Condensed matter and materials physics</title><description>We investigate the possibility of band structure engineering in the recently predicted 2D layered form of blue phosphorus via an electric field (E sub(z)) applied perpendicular to the layer(s). Using density functional theory, we study the effect of a transverse electric field in monolayer as well as three differently stacked bilayer structures of blue phosphorus. We find that for E sub(z) > 0.2 V/[Angstrom] the direct energy gap at the [Gamma] point, which is much larger than the default indirect band gap of mono- and bilayer blue phosphorus, decreases linearly with the increasing electric field, becomes comparable to the default indirect band gap at E sub(z) [asymptotically =] 0.45 (0.35) V/[Angstrom] for monolayer (bilayers), and decreases further until the semiconductor to metal transition of 2D blue phosphorus takes place at E sub(z) [asymptotically =] 0.7 (0.5) V/[Angstrom] for monolayer (bilayers). Calculated values of the electron and hole effective masses along various high symmetry directions in the reciprocal lattice suggests that the mobility of charge carriers is also influenced by the applied electric field.</description><subject>Asymptotic properties</subject><subject>Band structure of solids</subject><subject>Condensed matter</subject><subject>Electric fields</subject><subject>Monolayers</subject><subject>Phosphorus</subject><subject>Semiconductors</subject><subject>Two dimensional</subject><issn>1098-0121</issn><issn>1550-235X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNo1kEFLxDAQhYMouK7-AU89eumaaZK2Oeq6q8KCIgreQjpJbSS7rUkr7L83sjrwmMe8xxw-Qi6BLgAou37u9vHFft8uJKSD4IwdkRkIQfOCiffj5KmscwoFnJKzGD8pBS55MSN3K29xDA6z1llvMrczE1qTfegh2_bGtQ716PpdCrLJj0GPXXKNn2w2dH1MClM8Jyet9tFe_O05eVuvXpcP-ebp_nF5s8mRSTHmKApRo5YgjW4MR2CiLoxgBtCWlLeVbo1mFTWNkZJizZlhiEZbtEBLVrI5uTr8HUL_Ndk4qq2LaL3XO9tPUUFFZVWm4alaHKoY-hiDbdUQ3FaHvQKqfpGpf2RKgjogYz_04mJK</recordid><startdate>20150325</startdate><enddate>20150325</enddate><creator>Ghosh, Barun</creator><creator>Nahas, Suhas</creator><creator>Bhowmick, Somnath</creator><creator>Agarwal, Amit</creator><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20150325</creationdate><title>Electric field induced gap modification in ultrathin blue phosphorus</title><author>Ghosh, Barun ; Nahas, Suhas ; Bhowmick, Somnath ; Agarwal, Amit</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c395t-c5258ca919dabd4c13582d53d1ce604f7afda370dbd990c843d3ccdaece106363</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Asymptotic properties</topic><topic>Band structure of solids</topic><topic>Condensed matter</topic><topic>Electric fields</topic><topic>Monolayers</topic><topic>Phosphorus</topic><topic>Semiconductors</topic><topic>Two dimensional</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ghosh, Barun</creatorcontrib><creatorcontrib>Nahas, Suhas</creatorcontrib><creatorcontrib>Bhowmick, Somnath</creatorcontrib><creatorcontrib>Agarwal, Amit</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review. B, Condensed matter and materials physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ghosh, Barun</au><au>Nahas, Suhas</au><au>Bhowmick, Somnath</au><au>Agarwal, Amit</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Electric field induced gap modification in ultrathin blue phosphorus</atitle><jtitle>Physical review. B, Condensed matter and materials physics</jtitle><date>2015-03-25</date><risdate>2015</risdate><volume>91</volume><issue>11</issue><artnum>115433</artnum><issn>1098-0121</issn><eissn>1550-235X</eissn><abstract>We investigate the possibility of band structure engineering in the recently predicted 2D layered form of blue phosphorus via an electric field (E sub(z)) applied perpendicular to the layer(s). Using density functional theory, we study the effect of a transverse electric field in monolayer as well as three differently stacked bilayer structures of blue phosphorus. We find that for E sub(z) > 0.2 V/[Angstrom] the direct energy gap at the [Gamma] point, which is much larger than the default indirect band gap of mono- and bilayer blue phosphorus, decreases linearly with the increasing electric field, becomes comparable to the default indirect band gap at E sub(z) [asymptotically =] 0.45 (0.35) V/[Angstrom] for monolayer (bilayers), and decreases further until the semiconductor to metal transition of 2D blue phosphorus takes place at E sub(z) [asymptotically =] 0.7 (0.5) V/[Angstrom] for monolayer (bilayers). Calculated values of the electron and hole effective masses along various high symmetry directions in the reciprocal lattice suggests that the mobility of charge carriers is also influenced by the applied electric field.</abstract><doi>10.1103/PhysRevB.91.115433</doi></addata></record> |
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subjects | Asymptotic properties Band structure of solids Condensed matter Electric fields Monolayers Phosphorus Semiconductors Two dimensional |
title | Electric field induced gap modification in ultrathin blue phosphorus |
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