化工进展 ›› 2019, Vol. 38 ›› Issue (06): 2756-2767.DOI: 10.16085/j.issn.1000-6613.2018-1645
龙丹(),周俊伶,时洪民,王冠然,李红双,赵苾艺,李贞玉()
收稿日期:
2018-08-10
出版日期:
2019-06-05
发布日期:
2019-06-05
通讯作者:
李贞玉
作者简介:
龙丹(1993—),女,硕士研究生,研究方向为功能材料。E-mail:<email>danlong175201@163.com</email>。
基金资助:
Dan LONG(),Junling ZHOU,Hongmin SHI,Guanran WANG,Hongshuang LI,Biyi ZHAO,Zhenyu LI()
Received:
2018-08-10
Online:
2019-06-05
Published:
2019-06-05
Contact:
Zhenyu LI
摘要:
Cu2O是目前最有潜力的可见光光催化剂之一,在太阳能电池、一氧化碳氧化、光催化剂、传感器、化学模板等方面有着广泛的应用。然而,Cu2O光生电子-空穴对具有容易复合、易发生光腐蚀、稳定性不好等特性,使其在实际应用上面临很大的挑战,因此如何有效地提高Cu2O的光催化性能成为国内外研究者关注的焦点。首先,本文围绕Cu2O半导体的形貌控制、杂原子掺杂以及构建半导体异质结这三方面对Cu2O光催化性能的提升进行系统阐述,其中构建半导体异质结是提升Cu2O光催化性能最有效的方法,Cu2O与贵金属、金属氧化物以及碳材料构成的复合半导体异质结均有效地提高了Cu2O的光催化活性;其次,从复合半导体异质结、肖特基结以及Z-scheme机制三方面分析并讨论了Cu2O光催化增强机制;最后对Cu2O基纳米复合材料在电子结构、界面性质以及表面负载的成分和厚度等方面的研究进行了展望。
中图分类号:
龙丹, 周俊伶, 时洪民, 王冠然, 李红双, 赵苾艺, 李贞玉. 氧化亚铜光催化剂性能提升及增强机制的研究进展[J]. 化工进展, 2019, 38(06): 2756-2767.
Dan LONG, Junling ZHOU, Hongmin SHI, Guanran WANG, Hongshuang LI, Biyi ZHAO, Zhenyu LI. Research progress on the improved performance of cuprous oxide photocatalyst and its enhancement mechanism[J]. Chemical Industry and Engineering Progress, 2019, 38(06): 2756-2767.
光催化剂 | 添加量/mg | MO/mg·L-1 | 降解率/% | 光照时间/min | 光源 | 参考文献 | |
---|---|---|---|---|---|---|---|
Ni-Cu2O纳米线 | 20 | 20 | 94 | 80 | 300W 氙灯 (λ > 420nm) | [ | |
Cu@Cu2O核壳 | 4 | 20 | 90 | 100 | 太阳光(300~2500nm) | [ | |
中空Cu@Cu2O | 10 | 100 | 92 | 30 | 500W 氙灯 (λ > 400nm) | [ | |
Cu-Cu2O多面体 | 150 | 10 | 约为80 | 90 | 500W 氙灯(λ≥400nm) | [ | |
Au@Cu2O八面体 | 10.6 | 13 | 91 | 40 | 500W 氙灯(λ > 400nm) | [ | |
Ag/Cu2O类花状 | 40 | 30 | 81.2 | 40 | 500W 氙灯(λ > 400nm) | [ |
表1 不同形貌金属- Cu2O异质结构光催化剂的光降解MO的性能比较
光催化剂 | 添加量/mg | MO/mg·L-1 | 降解率/% | 光照时间/min | 光源 | 参考文献 | |
---|---|---|---|---|---|---|---|
Ni-Cu2O纳米线 | 20 | 20 | 94 | 80 | 300W 氙灯 (λ > 420nm) | [ | |
Cu@Cu2O核壳 | 4 | 20 | 90 | 100 | 太阳光(300~2500nm) | [ | |
中空Cu@Cu2O | 10 | 100 | 92 | 30 | 500W 氙灯 (λ > 400nm) | [ | |
Cu-Cu2O多面体 | 150 | 10 | 约为80 | 90 | 500W 氙灯(λ≥400nm) | [ | |
Au@Cu2O八面体 | 10.6 | 13 | 91 | 40 | 500W 氙灯(λ > 400nm) | [ | |
Ag/Cu2O类花状 | 40 | 30 | 81.2 | 40 | 500W 氙灯(λ > 400nm) | [ |
光催化剂 | E VB /eV | E CB/eV | E g/eV | 参考文献 | 光催 化剂 | E VB /eV | E CB/eV | E g/eV | 参考文献 |
---|---|---|---|---|---|---|---|---|---|
Ti2O | 2.91 | -0.29 | 3.2 | [ | Ag3PO4 | 2.67 | +0.25 | 2.42 | [ |
ZnO | 3.0 | -0.2 | 3.2 | [ | Bi2O3 | 3.13 | +0.33 | 2.8 | [ |
CdS | 1.88 | -0.52 | 2.4 | [ | C3N4 | 1.57 | -1.13 | 2.7 | [ |
Ce2O | 2.56 | -0.44 | 3.0 | [ | Cu2O | 0.9 | -1.3 | 2.2 | [ |
表2 对比几种常见的光催化剂能价带
光催化剂 | E VB /eV | E CB/eV | E g/eV | 参考文献 | 光催 化剂 | E VB /eV | E CB/eV | E g/eV | 参考文献 |
---|---|---|---|---|---|---|---|---|---|
Ti2O | 2.91 | -0.29 | 3.2 | [ | Ag3PO4 | 2.67 | +0.25 | 2.42 | [ |
ZnO | 3.0 | -0.2 | 3.2 | [ | Bi2O3 | 3.13 | +0.33 | 2.8 | [ |
CdS | 1.88 | -0.52 | 2.4 | [ | C3N4 | 1.57 | -1.13 | 2.7 | [ |
Ce2O | 2.56 | -0.44 | 3.0 | [ | Cu2O | 0.9 | -1.3 | 2.2 | [ |
光催化剂 | 制备 | 形貌 | 性能提升 | 增强机制 | 参考文献 |
---|---|---|---|---|---|
Cu2O/ZnO | 简单水热法和电沉积法 | 纳米棒 | 在可见光照射下5h后,Cu2O/ZnO对MO 的降解率是纯Cu2O纳米棒的20倍 | 增大了表面积;增强了光吸收范围;p-n异质结有效地分离了光生电子空穴对 | [ |
Cu2O/SrTiO3 | 溶胶-凝胶法和溶液还原法 | 纳米颗粒 | 在可见光下照射80min后,对MB 光降解率是Cu2O的3倍,是SrTiO3的1.5倍 | 形成p-n异质结加速光生电荷载体的 分离和迁移 | [ |
Cu2O/SnO2 | 简单的水热 浸渍法 | 纳米球 | 在可见光下照射90min后,对RhB 的降解速率比单个SnO2和混合相Cu2O高近2倍 | p-n结的形成增强了光响应;促进了光生电子空穴的分离;比表面积和孔隙率增大 | [ |
Cu2O/Bi2WO6 | 界面自组装法 | 类花状 | 在可见光下照射120min后,Cu2O/Bi2WO6对MB 的降解率是纯Bi2WO6和Cu2O的2.14倍和12.25倍 | 可见光吸收效率的提高;紧密接触界面中的强相互作用有效地提高光生电荷分离 | [ |
Cu2O/TiO2/ g-C3N4 | 简单的化学法 | 纳米颗粒(NPs) | 在可见光照射下,在3 ~ 15min可使 RhB、MB和MO变色 | 匹配能带以及p-n结的形成 | [ |
CQDs/Cu2O | 一步超声处理法 | 纳米球 | 在近红外光照下(λ> 700nm、240min),对MB 的降解率可达90%,而纯CQDs和Cu2O均不足3% | 形成肖特基能垒,阻止了光生电子- 空穴对的重组 | [ |
Au/Cu2O | 低温化学法;简单的化学法 | Au NPs沉积在Cu2O微晶表面 | 在可见光下照射90min,对MO 的光降解率以及光解水是纯Cu2O微球的1.2倍 | Au和Cu2O界面形成肖特基能垒,在内电场的作用下,有效地促进了光生电子和 空穴的分离 | [ |
Cu2O/Ag3PO4 | 简单的化学法 | 八面体 | 在可见光照射下(8min)对MB 的光降解速率分别为Cu2O和Ag3PO4的7倍和2.1倍 | Z-scheme机理;光生载流子的有效分离 | [ |
Cu2O/Cu/g-C3N4 | 一步还原法 | Cu2O/Cu NPs沉积在g-C3N4表面 | 在可见光照射下(60min),对MO的光催化降解率分别是P25 TiO2、g-C3N4和Cu2O/Cu的9倍、3.3倍和2倍 | Z-scheme电荷转移机理;Cu 为电荷分离中心 | [ |
表3 不同光降解机制的对比
光催化剂 | 制备 | 形貌 | 性能提升 | 增强机制 | 参考文献 |
---|---|---|---|---|---|
Cu2O/ZnO | 简单水热法和电沉积法 | 纳米棒 | 在可见光照射下5h后,Cu2O/ZnO对MO 的降解率是纯Cu2O纳米棒的20倍 | 增大了表面积;增强了光吸收范围;p-n异质结有效地分离了光生电子空穴对 | [ |
Cu2O/SrTiO3 | 溶胶-凝胶法和溶液还原法 | 纳米颗粒 | 在可见光下照射80min后,对MB 光降解率是Cu2O的3倍,是SrTiO3的1.5倍 | 形成p-n异质结加速光生电荷载体的 分离和迁移 | [ |
Cu2O/SnO2 | 简单的水热 浸渍法 | 纳米球 | 在可见光下照射90min后,对RhB 的降解速率比单个SnO2和混合相Cu2O高近2倍 | p-n结的形成增强了光响应;促进了光生电子空穴的分离;比表面积和孔隙率增大 | [ |
Cu2O/Bi2WO6 | 界面自组装法 | 类花状 | 在可见光下照射120min后,Cu2O/Bi2WO6对MB 的降解率是纯Bi2WO6和Cu2O的2.14倍和12.25倍 | 可见光吸收效率的提高;紧密接触界面中的强相互作用有效地提高光生电荷分离 | [ |
Cu2O/TiO2/ g-C3N4 | 简单的化学法 | 纳米颗粒(NPs) | 在可见光照射下,在3 ~ 15min可使 RhB、MB和MO变色 | 匹配能带以及p-n结的形成 | [ |
CQDs/Cu2O | 一步超声处理法 | 纳米球 | 在近红外光照下(λ> 700nm、240min),对MB 的降解率可达90%,而纯CQDs和Cu2O均不足3% | 形成肖特基能垒,阻止了光生电子- 空穴对的重组 | [ |
Au/Cu2O | 低温化学法;简单的化学法 | Au NPs沉积在Cu2O微晶表面 | 在可见光下照射90min,对MO 的光降解率以及光解水是纯Cu2O微球的1.2倍 | Au和Cu2O界面形成肖特基能垒,在内电场的作用下,有效地促进了光生电子和 空穴的分离 | [ |
Cu2O/Ag3PO4 | 简单的化学法 | 八面体 | 在可见光照射下(8min)对MB 的光降解速率分别为Cu2O和Ag3PO4的7倍和2.1倍 | Z-scheme机理;光生载流子的有效分离 | [ |
Cu2O/Cu/g-C3N4 | 一步还原法 | Cu2O/Cu NPs沉积在g-C3N4表面 | 在可见光照射下(60min),对MO的光催化降解率分别是P25 TiO2、g-C3N4和Cu2O/Cu的9倍、3.3倍和2倍 | Z-scheme电荷转移机理;Cu 为电荷分离中心 | [ |
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