偶氮苯类衍生物用于非线性光学材料的理论研究

 2023-07-31 08:36:04

论文总字数:25494字

摘 要

:采用密度泛函理论(DFT)基于B3LYP/6-311 G**、B3LYP /6-311G**两种计算方法对实验合成的偶氮苯系列衍生物的分子结构进行了优化,探讨了具有不同取代基的偶氮苯衍生物的红外光谱(IR),紫外光谱(UV),前线分子轨道及非线性光学(NLO)性质,结果表明偶氮苯衍生物分子具有很好的共轭性,N=N双键在分子中起到了很好的电子传递作用,分子所呈现的极性较大。通过对比发现,具有供电子基-OCH3的化合物的NLO 系数明显高于Cl-取代基的化合物。同时对化合物的IR光谱进行了归属分析。

关键词:偶氮苯衍生物,非线性光学性质,DFT

Abstract: The molecular structure of the experimentally synthesized azobenzene derivatives were optimized by using density functional theory (DFT) based on two methods of B3LYP/6-311 G**、B3LYP /6-311G**. And we discussed the infrared spectrum(IR), ultraviolet spectrum(UV), frontier molecular orbital and nonlinear optical (NLO) of the Azobenzene derivatives with different substituents. The results show that azobenzene derivatives have good conjugation, and N=N double bond in the molecule plays a very good electron transfer. The molecules present a large polarity. By comparison, we find that the nonlinear optical coefficient of the compound with electron donating group -OCH3 was significantly higher than that with Cl- substituents. At the same time, the IR spectrum of the compound was analyzed.

Keywords: azobenzene derivative, nonlinear optical properties, dft

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目 录

1 前言 4

1.1 非线性光学材料的研究现状及应用前景 4

1.2 偶氮苯及其衍生物的非线性光学性质研究 4

2 计算方法 4

3 结果与讨论 5

3.1 分子几何构型 5

3.2 红外光谱 10

3.2.1 C-H振动 14

3.2.2 苯环及杂芳环的骨架振动 14

3.2.3 C-O伸缩振动 15

3.3 前线分子轨道分析 15

3.4 非线性光学性质 17

结论 19

参考文献 21

致谢 22

1 前言

1.1 非线性光学材料的发展及应用前景

非线性光学是当代光学领域的一部分,其探究的是物质在激光这样的强相干光束照射下产生响应,而使折射率等光学现象发生变化的现象。1960年代,弗兰肯等人用红宝石激光束所得到的强光束通过石英晶体时产生了二次谐波,而基频光频率是光波频率的1/2,首次发现了倍频现象[1-3]。这一发现开创了非线性光学及其物质载体的研究范畴。通过研究我们发现,具有非对称的电荷分布、大的π电子共轭体系、大的极化率的分子构成的物质即可作为非线性光学材料。可以作为非线性光学材料的晶体一般有几种:无机晶体、有机晶体、无机-有机杂化晶体、金属有机晶体。无机晶体中,KDP 型晶体、KTP型晶体、钙钛矿型晶体、沸石分子筛基材料、玻璃非线性光学材料、半导体、硼酸盐晶体等具有晶体纯度高、各项异性、稳定的性质,被广泛用于非线性光学材料[4]。有机晶体因其具有结构多样化、非线性极化率高、可变性强、光学响应速度快[5-7]等优点,引起化学工作者们的注意,从而被探索研究,广泛应用于非线性光学材料[8]

1.2 偶氮苯及其衍生物作为非线性光学材料的研究

偶氮苯类化合物属于芳香族含氮物,具有可进入显色光区的π电子,是应用最广、颜色种类最多的一种合成染料。偶氮苯在强烈的光照条件下可翻转成顺式,而在一定条件下又能可逆地翻转成反式,这种光致异构的现象受到广泛关注,并被应用于分子光控开关[9]、全息记录器件、分子机器人等领域。通过研究我们发现偶氮苯类化合物存在着能使电子自由流动的N=N,从而使其容易产生NLO效应[10]。曾艺、潘志华等人实验合成了偶氮类衍生物azo12-MO,兼有甲基橙和液晶类聚合物azo12的特点,通过测算发现其非线性光学性质要优于甲基橙azo12[11]。蒋爱国等人采用量子化学方法探讨了2-氨基噻唑偶氮苯衍生物的二阶非线性光学(NLO) 性质[12],本文于李巍巍实验合成的2,4-二氯-6-偶氮苯氧基-1,3,5均三嗪(L1)[13]与2,4-二甲氧基-6-偶氮苯氧基-1,3,5均三嗪(L2)基础上,采用DFT理论将分子构型优化,从理论上研究其分子结构和光学性质关系,分析不同基团对其NLO性质产生的影响。

2 计算方法

本文采用密度泛函(DFT)B3LYP方法,于6-311 G**、6-311G**两种基组上对分子进行几何构型的优化与计算,得到具有稳定构型的结构。构型优化是理论计算中最重要的步骤之一。计算分两步进行,第一步采用Hyperchem 6.0软件包建立化合物的初始构型,用MM 分子动力学对几何构型进行优化,当分子处于最低能量时即默认为收敛值。第二步,将优化结果采用DFT B3LYP方法分别在6-311 G**和6-311G**基组上进行优化处理。同样的,分子HOMO、LUMO轨道能量与跃迁和分子极化率β值的计算都是基于以上方法。电子性质的计算采取含时密度泛函理论TD-DFT方法。所有计算都在Gaussian 09W 程序中完成。

3 结果与讨论

3.1 分子几何构型

图1 L1分子的优化几何结构

图2 L2分子的优化几何结构

表1 L1、L2分子计算所得键长、键角、及二面角

L1

L2

B3LYP

6-311 G**

6-311G**

6-311 G**

6-311G**

R(1,2)

1.3921

1.3913

R(1,2)

1.3922

1.3914

R(1,3)

1.3934

1.393

R(1,3)

1.3934

1.3930

R(1,4)

1.0839

1.0838

R(1,4)

1.0839

1.0839

R(2,5)

1.3991

1.3987

R(2,5)

1.3991

1.3985

R(2,7)

1.0836

1.0834

R(2,7)

1.0837

1.0834

R(3,6)

1.3991

1.3985

R(3,6)

1.3989

1.3984

R(3,8)

1.0842

1.0842

R(3,8)

1.0842

1.0842

R(5,9)

1.4038

1.4032

R(5,9)

1.4037

1.4031

R(5,11)

1.4181

1.4169

R(5,11)

1.4187

1.4178

R(6,9)

1.3877

1.3868

R(6,9)

1.3879

1.3870

R(6,10)

1.0843

1.0843

R(6,10)

1.0844

1.0843

R(9,12)

1.0819

1.0817

R(9,12)

1.0820

1.0817

R(11,13)

1.2522

1.2541

R(11,13)

1.2526

1.2538

R(13,14)

1.4188

1.4157

R(13,14)

1.4175

1.4165

R(14,15)

1.3984

1.3954

R(14,15)

1.3989

1.3985

R(14,16)

1.4035

1.4042

R(14,16)

1.4039

1.4034

R(15,18)

1.3911

1.3931

R(15,18)

1.3908

1.3899

R(15,20)

1.0832

1.0832

R(15,20)

1.0834

1.0831

R(16,17)

1.3865

1.3811

R(16,17)

1.3863

1.3853

R(16,19)

1.0817

1.0814

R(16,19)

1.0819

1.0816

R(17,21)

1.3918

1.4001

R(17,21)

1.3940

1.3941

R(17,23)

1.0833

1.0828

R(17,23)

1.0834

1.0832

R(18,21)

1.3861

1.3922

R(18,21)

1.3881

1.3884

R(18,22)

1.0828

1.0764

R(18,22)

1.0829

1.0827

R(21,24)

1.4062

1.3977

R(21,24)

1.3963

1.3950

R(24,25)

1.3322

1.3265

R(24,25)

1.3471

1.3480

R(25,26)

1.3364

1.3408

R(25,26)

1.3207

1.3204

R(25,27)

1.3335

1.3332

R(25,27)

1.3352

1.3343

R(26,29)

1.3181

1.3143

R(26,29)

1.3375

1.3377

R(27,28)

1.323

1.3243

R(27,28)

1.3322

1.3320

R(28,30)

1.3251

1.3212

R(28,30)

1.3341

1.3337

R(28,31)

1.7370

1.7407

R(28,31)

1.3293

1.3287

R(29,30)

1.3313

1.3338

R(29,30)

1.3313

1.3309

R(29,32)

1.7368

1.7394

R(29,32)

1.3289

1.3285

R(31,33)

1.4395

1.4386

R(32,34)

1.4387

1.4376

R(33,37)

1.0877

1.0877

R(33,38)

1.0904

1.0906

R(33,39)

1.0904

1.0906

R(34,35)

1.0905

1.0907

R(34,36)

1.0878

1.0878

R(34,40)

1.0905

1.0907

A(2,1,3)

119.8491

119.8255

A(2,1,3)

119.868

119.8388

A(2,1,4)

119.9693

119.9792

A(2,1,4)

119.9574

119.9755

A(3,1,4)

120.1816

120.1953

A(3,1,4)

120.1746

120.1857

A(1,2,5)

120.1516

120.2197

A(1,2,5)

120.1863

120.2381

A(1,2,7)

121.3608

121.5219

A(1,2,7)

121.3478

121.5239

A(5,2,7)

118.4876

118.2584

A(5,2,7)

118.4659

118.2379

A(1,3,6)

120.0379

120.049

A(1,3,6)

119.9930

120.0212

A(1,3,8)

120.0542

120.0368

A(1,3,8)

120.0750

120.0527

A(6,3,8)

119.9079

119.9142

A(6,3,8)

119.9320

119.9262

A(2,5,9)

119.9943

119.8864

A(2,5,9)

119.9337

119.8524

A(2,5,11)

115.4060

115.5313

A(2,5,11)

115.4377

115.5340

A(9,5,11)

124.5997

124.5823

A(9,5,11)

124.6286

124.6136

A(3,6,9)

120.4644

120.4173

A(3,6,9)

120.4807

120.4215

A(3,6,10)

119.7965

119.8171

A(3,6,10)

119.7925

119.8186

A(9,6,10)

119.7391

119.7656

A(9,6,10)

119.7268

119.7598

A(5,9,6)

119.5026

119.6022

A(5,9,6)

119.5382

119.6280

A(5,9,12)

119.1996

118.8527

A(5,9,12)

119.1681

118.8217

A(6,9,12)

121.2978

121.5451

A(6,9,12)

121.2937

121.5503

A(5,11,13)

115.5100

115.2662

A(5,11,13)

115.4347

115.2237

A(11,13,14)

115.2020

114.9638

A(11,13,14)

115.3550

115.1491

A(13,14,15)

115.5077

115.9160

A(13,14,15)

115.5585

115.6542

A(13,14,16)

124.6185

124.7627

A(13,14,16)

124.6730

124.6589

A(15,14,16)

119.8733

119.3213

A(15,14,16)

119.7677

119.6860

A(14,15,18)

120.4701

121.5886

A(14,15,18)

120.4887

120.5353

A(14,15,20)

118.6136

118.2510

A(14,15,20)

118.5536

118.3204

A(18,15,20)

120.9161

120.1604

A(18,15,20)

120.9575

121.1441

A(14,16,17)

119.8668

119.7721

A(14,16,17)

119.8550

119.9392

A(14,16,19)

119.2056

119.0706

A(14,16,19)

119.1820

118.8290

A(17,16,19)

120.9274

121.1573

A(17,16,19)

120.9626

121.2317

A(16,17,21)

119.1566

120.0388

A(16,17,21)

119.4888

119.4923

A(16,17,23)

121.1194

121.4770

A(16,17,23)

121.1278

121.2125

A(21,17,23)

119.7238

118.4841

A(21,17,23)

119.3829

119.2941

A(15,18,21)

118.5897

118.0594

A(15,18,21)

118.8975

118.9306

A(15,18,22)

121.3665

120.9035

A(15,18,22)

121.3507

121.4215

A(21,18,22)

120.0436

121.0371

A(21,18,22)

119.7514

119.6469

A(17,21,18)

122.0378

121.2197

A(17,21,18)

121.4932

121.4119

A(17,21,24)

118.9268

111.8759

A(17,21,24)

119.0747

119.1287

A(18,21,24)

118.8476

126.9041

A(18,21,24)

119.2288

119.2770

A(21,24,25)

120.0709

129.1648

A(21,24,25)

119.9273

119.7655

A(24,25,26)

114.4586

112.8785

A(24,25,26)

114.4411

114.3759

A(24,25,27)

119.7369

121.9643

A(24,25,27)

118.5148

118.4620

A(26,25,27)

125.8044

125.1572

A(26,25,27)

127.0441

127.1621

A(25,26,29)

113.4695

113.7925

A(25,26,29)

113.1869

113.0421

A(25,27,28)

113.6338

113.8730

A(25,27,28)

113.5277

113.4973

A(27,28,30)

127.0188

127.2750

A(27,28,30)

126.0023

126.0114

A(27,28,31)

116.5331

116.1915

A(27,28,31)

119.2383

119.2170

A(30,28,31)

116.448

116.5335

A(30,28,31)

114.7595

114.7716

A(26,29,30)

127.2061

127.3388

A(26,29,30)

126.5047

126.6037

A(26,29,32)

116.6877

116.7555

A(26,29,32)

114.3573

114.2953

A(30,29,32)

116.1062

115.9057

A(30,29,32)

119.1379

119.1011

A(28,30,29)

112.8674

112.5635

A(28,30,29)

113.7344

113.6834

A(28,31,33)

118.0585

117.7912

A(29,32,34)

118.0720

117.7825

A(31,33,37)

104.8201

104.868

A(31,33,38)

110.6731

110.7597

A(31,33,39)

110.7096

110.7916

A(37,33,38)

110.6474

110.6489

A(37,33,39)

110.6762

110.6752

A(38,33,39)

109.2629

109.0593

A(32,34,35)

110.6802

110.7633

A(32,34,36)

104.7965

104.8702

A(32,34,40)

110.6918

110.7720

A(35,34,36)

110.6946

110.6835

A(35,34,40)

109.2314

109.0298

A(36,34,40)

110.6963

110.6858

D(3,1,2,5)

0.0177

0.0031

D(3,1,2,5)

0.0081

0.0011

D(3,1,2,7)

-179.9673

-179.9949

D(3,1,2,7)

-179.9843

-179.9847

D(4,1,2,5)

179.9903

-179.9991

D(4,1,2,5)

179.9991

179.991

D(4,1,2,7)

0.0053

0.0029

D(4,1,2,7)

0.0067

0.0053

D(2,1,3,6)

-0.0133

-0.0003

D(2,1,3,6)

0.0189

0.0144

D(2,1,3,8)

179.9667

179.9996

D(2,1,3,8)

-179.9948

179.9940

D(4,1,3,6)

-179.9859

-179.9982

D(4,1,3,6)

-179.9721

-179.9755

D(4,1,3,8)

-0.0059

0.0018

D(4,1,3,8)

0.0142

0.0041

D(1,2,5,9)

-0.0157

-0.0044

D(1,2,5,9)

-0.0402

-0.0183

D(1,2,5,11)

-179.9565

-179.9941

D(1,2,5,11)

179.9206

179.9590

D(7,2,5,9)

179.9697

179.9937

D(7,2,5,9)

179.9525

179.9679

D(7,2,5,11)

0.0289

0.0039

D(7,2,5,11)

-0.0868

-0.0548

D(1,3,6,9)

0.0071

-0.0011

D(1,3,6,9)

-0.0139

-0.0127

D(1,3,6,10)

179.9864

179.9992

D(1,3,6,10)

179.9548

179.9651

D(8,3,6,9)

-179.973

179.9989

D(8,3,6,9)

179.9998

-179.9924

D(8,3,6,10)

0.0063

-0.0007

D(8,3,6,10)

-0.0315

-0.0146

D(2,5,9,6)

0.0093

0.0029

D(2,5,9,6)

0.0449

0.0200

D(2,5,9,12)

-179.9699

-179.9941

D(2,5,9,12)

-179.9416

-179.9621

D(11,5,9,6)

179.9444

179.9917

D(11,5,9,6)

-179.9120

-179.9551

D(11,5,9,12)

-0.0348

-0.0054

D(11,5,9,12)

0.1015

0.0628

D(2,5,11,13)

-179.7657

-179.9391

D(2,5,11,13)

-179.8240

-179.897

D(9,5,11,13)

0.2965

0.0716

D(9,5,11,13)

0.1347

0.0790

D(3,6,9,5)

-0.0051

-0.0002

D(3,6,9,5)

-0.0180

-0.0046

D(3,6,9,12)

179.9737

179.9968

D(3,6,9,12)

179.9682

179.9770

D(10,6,9,5)

-179.9844

179.9995

D(10,6,9,5)

-179.9868

-179.9823

D(10,6,9,12)

-0.0056

-0.0036

D(10,6,9,12)

-0.0006

-0.0007

D(5,11,13,14)

-179.8965

-179.9982

D(5,11,13,14)

179.9199

179.9484

D(11,13,14,15)

-179.6077

-179.9058

D(11,13,14,15)

-179.3247

-179.6274

D(11,13,14,16)

0.1471

0.0858

D(11,13,14,16)

0.9973

0.7188

D(13,14,15,18)

179.9549

179.9871

D(13,14,15,18)

179.7831

179.8808

D(13,14,15,20)

0.1338

-0.0034

D(13,14,15,20)

-0.3765

-0.2260

D(16,14,15,18)

0.1876

-0.0050

D(16,14,15,18)

-0.5220

-0.4470

D(16,14,15,20)

-179.6335

-179.9956

D(16,14,15,20)

179.3184

179.4461

D(13,14,16,17)

-179.9533

-179.9862

D(13,14,16,17)

-179.8403

-179.928

D(13,14,16,19)

-0.1421

0.0018

D(13,14,16,19)

0.3871

0.2131

D(15,14,16,17)

-0.2085

0.0052

D(15,14,16,17)

0.4944

0.4313

D(15,14,16,19)

179.6027

179.9932

D(15,14,16,19)

-179.2783

-179.4277

D(14,15,18,21)

0.3395

0.0184

D(14,15,18,21)

-0.2008

-0.0886

D(14,15,18,22)

-179.5133

179.9403

D(14,15,18,22)

179.567

179.5542

D(20,15,18,21)

-179.8436

-179.9913

D(20,15,18,21)

179.9627

-179.9787

D(20,15,18,22)

0.3037

-0.0693

D(20,15,18,22)

-0.2695

-0.3359

D(14,16,17,21)

-0.2975

-0.0189

D(14,16,17,21)

0.2521

0.1170

D(14,16,17,23)

179.5522

179.979

D(14,16,17,23)

-179.4862

-179.4945

D(19,16,17,21)

179.8946

179.9933

D(19,16,17,21)

-179.9794

179.9725

D(19,16,17,23)

-0.2557

-0.0088

D(19,16,17,23)

0.2824

0.3609

D(16,17,21,18)

0.8537

0.0332

D(16,17,21,18)

-1.0001

-0.6692

D(16,17,21,24)

175.813

179.8492

D(16,17,21,24)

-175.7772

-175.7260

D(23,17,21,18)

-178.9982

-179.9648

D(23,17,21,18)

178.7428

178.9498

D(23,17,21,24)

-4.0389

-0.1488

D(23,17,21,24)

3.9656

3.8931

D(15,18,21,17)

-0.8707

-0.0323

D(15,18,21,17)

0.9704

0.6527

D(15,18,21,24)

-175.8339

-179.8188

D(15,18,21,24)

175.7396

175.7022

D(22,18,21,17)

178.984

-179.9542

D(22,18,21,17)

-178.8012

-178.9966

D(22,18,21,24)

4.0208

0.2593

D(22,18,21,24)

-4.0319

-3.9470

D(17,21,24,25)

90.226

178.8493

D(17,21,24,25)

-91.8231

-91.8875

D(18,21,24,25)

-94.6519

-1.3474

D(18,21,24,25)

93.2799

92.9489

D(21,24,25,26)

-179.6603

-179.9183

D(21,24,25,26)

179.6712

179.7475

D(21,24,25,27)

0.4244

0.0569

D(21,24,25,27)

-0.3775

-0.2903

D(24,25,26,29)

-179.9052

179.9666

D(24,25,26,29)

179.9738

179.9756

D(27,25,26,29)

0.0042

-0.0077

D(27,25,26,29)

0.0274

0.0172

D(24,25,27,28)

179.8837

-179.9630

D(24,25,27,28)

-179.9487

-179.9508

D(26,25,27,28)

-0.0213

0.0090

D(26,25,27,28)

-0.0043

0.0060

D(25,26,29,30)

0.0076

0.0006

D(25,26,29,30)

-0.0232

-0.0269

D(25,26,29,32)

-179.9965

179.9992

D(25,26,29,32)

179.981

179.9844

D(25,27,28,30)

0.0307

-0.0037

D(25,27,28,30)

-0.0280

-0.0247

D(25,27,28,31)

-179.9657

-179.9956

D(25,27,28,31)

179.9526

179.9486

D(27,28,30,29)

-0.0209

-0.0022

D(27,28,30,29)

0.0314

0.0167

D(31,28,30,29)

179.9754

179.9897

D(31,28,30,29)

-179.9501

-179.9576

D(26,29,30,28)

-0.0001

0.0038

D(27,28,31,33)

-0.1575

-0.1236

D(32,29,30,28)

180.0039

-179.9947

D(30,28,31,33)

179.8253

179.8527

D(26,29,30,28)

-0.0033

0.0115

D(32,29,30,28)

179.9923

-180.0002

D(26,29,32,34)

179.9461

179.9613

D(30,29,32,34)

-0.0500

-0.0283

D(28,31,33,37)

179.8244

179.8623

D(28,31,33,38)

-60.8554

-60.7431

D(28,31,33,39)

60.4513

60.4199

D(29,32,34,35)

-60.6638

-60.6072

D(29,32,34,36)

179.9701

179.9539

D(29,32,34,40)

60.5960

60.5077

L1、L2分子最优几何构型与原子编号如图1、图2所示,表1给出了两个分子稳定构型的键长、键角和二面角。从表1的数据可以看出,L1分子中的C5-N11、C14-N13键长略小于L2分子,而N11=N13 双键略长于L2分子,电子流通性更好。L1分子C21-O24键长略长于L2分子,而C25-O24键长小于L2分子,这是由于杂环上的取代基不一样,导致具有Cl离子取代基的L1分子共轭体系范围扩大,键长趋于平均化,电子流通性优于L2分子。通过计算可知L1分子的C-Cl键键长在1.738 Å左右,符合典型的C-Cl键。L2分子C28-O31和C29-O32键长在1.328 Å左右,符合典型的C-O键。通过B3LYP/6-311 G**、B3LYP /6-311G**两种计算方法L1分子C21-O24-C25键角和大于L2分子,可以知道,具有Cl-取代基的L1分子更趋于平面,所以共轭体系范围扩大,电子流通性更好。

3.2 红外光谱

表2 L1、L2分子通过B3LYP/6-311 G**、B3LYP/6-311G**计算所得的红外振动频率值

L1

L2

B3LYP

6-311 G**

6-311G**

B3LYP

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