Gap Structure of the Overdoped Iron-Pnictide Superconductor Ba(Fe<sub>0.942</sub>Ni<sub>0.058</sub>)<sub>2</sub>As<sub>2</sub>: A Low-Temperature Specific-Heat Study

<div>The raw data (color online) of the SH under different fields in the low temperature region. The data are shown in <svg height="11.9171pt" id="M36" style="vertical-align:-2.2392pt" version="1.1" viewbox="-0.0498162 -9.6779 23.4491 11.9171" width="23.4491pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><g transform="matrix(.0135,0,0,-0.0135,0,0)"><path d="M645 631C614 643 545 666 457 666C215 666 23 519 23 283C23 90 158 -16 337 -16C412 -16 489 2 522 10C543 39 590 127 606 167L580 181C519 89 459 18 348 18C201 18 122 136 122 287C122 464 244 632 435 632C544 632 602 595 608 472L639 475C643 526 645 581 645 631Z" id="g113-68"></path><glyph.data ascent="3473" descent="-2876" horiz-adv-x="668" vert-adv-y="668"></glyph.data></g><g transform="matrix(.0135,0,0,-0.0135,9.05,0)"><path d="M368 703H309L44 -163H104L368 703Z" id="g113-48"></path><glyph.data ascent="3473" descent="-2876" horiz-adv-x="412" vert-adv-y="412"></glyph.data></g><g transform="matrix(.0135,0,0,-0.0135,14.638,0)"><path d="M620 675H597C578 656 570 650 541 650H144C112 650 104 653 94 675H72C59 618 42 552 23 493L53 491C71 534 88 564 105 585C124 608 144 615 238 615H290L197 121C182 40 174 34 88 28L82 0H361L367 28C275 34 266 38 281 121L374 615H441C522 615 543 608 553 583C562 560 566 531 565 493L597 494C603 551 612 629 620 675Z" id="g113-85"></path><glyph.data ascent="3473" descent="-2876" horiz-adv-x="637" vert-adv-y="637"></glyph.data></g></svg> versus <svg height="12.1279pt" id="M37" style="vertical-align:-0.04979992pt" version="1.1" viewbox="-0.0498162 -12.0781 13.8962 12.1279" width="13.8962pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><g transform="matrix(.0135,0,0,-0.0135,0,0)"><path d="M620 675H597C578 656 570 650 541 650H144C112 650 104 653 94 675H72C59 618 42 552 23 493L53 491C71 534 88 564 105 585C124 608 144 615 238 615H290L197 121C182 40 174 34 88 28L82 0H361L367 28C275 34 266 38 281 121L374 615H441C522 615 543 608 553 583C562 560 566 531 565 493L597 494C603 551 612 629 620 675Z" id="g113-85"></path><glyph.data ascent="3473" descent="-2876" horiz-adv-x="637" vert-adv-y="637"></glyph.data></g><g transform="matrix(.0095,0,0,-0.0095,8.635,-5.984)"><path d="M414 144C384 79 371 75 317 75H135L276 221C367 316 408 376 408 465C408 570 327 635 237 635C179 635 131 609 100 575L42 494L67 471C94 510 138 565 205 565C277 565 321 517 321 435C321 348 258 270 195 195C146 137 88 81 33 26V0H411C423 44 433 88 446 135L414 144Z" id="g50-51"></path><glyph.data ascent="3443" descent="-2856" horiz-adv-x="487" vert-adv-y="487"></glyph.data></g></svg> plot. The solid lines display the theoretical fitting (see text). The dashed straight line is the guide for the eyes.</div>

Advances in Condensed Matter Physics

fig3

Figure 3

Figure 3: Gap Structure of the Overdoped Iron-Pnictide Superconductor Ba(Fe<sub>0.942</sub>Ni<sub>0.058</sub>)<sub>2</sub>As<sub>2</sub>: A Low-Temperature Specific-Heat Study 

Advances in Condensed Matter Physics

Gap Structure of the Overdoped Iron-Pnictide Superconductor Ba(Fe0.942Ni0.058)2As2: A Low-Temperature Specific-Heat Study

Figure 3

Gap Structure of the Overdoped Iron-Pnictide Superconductor Ba(Fe_0.942Ni_0.058)₂As₂: A Low-Temperature Specific-Heat Study