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Tóm tắt luận án Tiến sĩ Vật lý: Nghiên cứu các tính chất động học và phát triển hệ laser rắn tử ngoại sử dụng vật liệu pha tạp ion Ce3+

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Luận văn tiến hành nhằm nghiên cứu các quá trình động học phát xạ cho laser rắn tử ngoại Ce:LiCAF băng rộng, có khả năng phát đơn xung ngắn dưới nano giây. Đánh giá ảnh hưởng của năng lượng laser bơm, thông số BCH lên độ rộng xung laser lối ra. Mời các bạn cùng tham khảo nội dung chi tiết.

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MINISTRY OF EDUCATION

AND TRAINING

VIETNAM ACADEMYOF SCIENCE AND TECHNOLOGY

GRADUATE UNIVERSITY SCIENCE AND

TECHNOLOGY -

NGUYEN THI MAI THO

STUDY ON USING PHOTOTCATALYST BASED

O N L A Y E R E D D O U B L E H Y D R O X I D E S ZnBi2O4/GRAPHIT AND ZnBi2O4/Bi2S3 FOR

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The dissertation was completed at: Industrial University of Ho Chi Minh City, Korea Instite of Toxicology – Gajeong-ro, Yuseong-gu, Daejeon; The Department of Chemistry - Changwon National University; HoChiMinh City Institute of Resources Geography Graduate University of Sciences and Technology, Vietnam Academy

of Science and Technology; Institute of Applied Materials Science Scientific Supervisors:

1 Assoc Prof Dr Nguyen Thi Kim Phuong

2 Dr Bui The Huy

At … hour… date… month … 2021

The dissertation can be found in:

- National Library of Vietnam and the library of Graduate University

of Science And Technology

- Vietnam Academy of Science and Technology

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INTRODUCTION

1 The necessity of the thesis

Currently, environmental pollution is at an alarming level, especially pollution of textile industry wastewater Therefore, the research and development of materials as well as the textile and dyeing wastewater treatment methods are essential requirements The removal of harmful organic pollutants through advanced oxidation processes (AOPs) photocatalytic oxidation is attracting an increasing attention Heterojunctions in photocatalysts has been proved to be one of the most promising ways for the preparation of advanced photocatalysts because of its feasibility and effectiveness for the spatial separation of electron–hole pairs

2 Objectives

Study on treatment of RhB (Rhodamine B) and IC (Indigo carmine) dyes by photocatalytic ZnBi2O4/x.0Graphite, ZnBi2O4/x.0Bi2S3 under visible light

3 Research scope and content

ZnBi2O4/x.0Graphite and ZnBi2O4/x.0Bi2S3 composites have signifcance to find cost-effective and advanced heterojunction photocatalysts for environmental remediation

4 Structure of the thesis

The dissertation has 116 pages, including the Preface, Chapter 1: Overview, Chapter 2: Experiment, Chapter 3: Results and discussions, Conclusions, publications with 44 images, 32 tables and 153 references

Chapter 1 OVERVIEW

A heterojunction, in general, is defned as the interface between two different semiconductors with unequal band structure, which can

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result in band alignments The heterojunction photocatalyst should fulft several requirements, such as visible-light activity, high solar-conversion effciency, proper bandgap structure for redox reactions, high photostability for long-term applications, and scalability for commercialization Many semiconductors have been investigated and developed for various photocatalytic such as ZnO/Al-Mg-LDHs, RGO/Bi-Zn-LDHs,Ti/ZnO-Cr2O3

Recently, mixed-metal oxides, which are prepared by the calcination treatment of layered double hydroxides (LDHs), have been used as photocatalysts for the elimination of toxic organic compounds in aqueous solutions LDHs are two-dimensional layered anionic clays that are generally expressed as [M1-x2+Mx3+ (OH)2]x+ (An-)x/n.yH2O as one of the simplest mixed-metal oxides derived from LDHs, ZnBi2O4

is a promising, highly efficient, visible-light active photocatalyst, with advantages of small optical band gap, high stability, and low conduction band edges There have been many studies of the photocatalysts application based on Bi3+to remove organic pollutants Graphite is a carbon allotrope with a layered structure of stacked graphene sheets It is commonly available and widely used as an adsorbent for organic pollutants and several studies on the photocatalytic performance of graphite have been reported so far Bismuth sulfide (Bi2S3) has a typical lamellar structure with a narrow bandgap, especially as a potential visible light photocatalyst through combination with other semiconductors material

In the present work, ZnBi2O4/x.0Graphite and ZnBi2O4/x.0Bi2S3 composites were obtained through a simple co-precipitation method which exhibited effective photocatalysis for the decomposition of RhB and IC under visible light

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Chapter 2 EXPERIMENT

2.1 Synthetic of ZnBi 2 O 4 /x.0Graphite and ZnBi 2 O 4 /x.0Bi 2 S 3

Synthesized ZnBi2O4/x.0Graphite and ZnBi2O4/x.0Bi2S3

heterojunction by in-situ coprecipitation (Figure 2.1) The as-prepared materials were labeled as ZnBi2O4, ZnBi2O4/x.0Graphite (x = 1, 2, 5,

10, and 20), ZnBi2O4/x.0Bi2S3(x = 1, 2, 6, 12, and 20), x is the

percentages of graphite and Bi2S3 in ZnBi2O4

Figure 2.1 The synthesis process a) ZnBi 2 O 4 /x.0Graphit and

(b) ZnBi2O4/x.0Bi2S3

The ZnBi2O4/x.0Graphite and ZnBi2O4/x.0Bi2S3 were characterized using various methods, including XRD, IR, XPS, UV-VIS, SEM, TEM, UV-Vis DRS

2.2 Applications of ZnBi 2 O 4 /x.0Graphite and ZnBi 2 O 4 /x.0Bi 2 S 3 photocatalytic systems

The photocatalytic activity of the ZnBi2O4/x.0Graphite and ZnBi2O4/x.0Bi2S3 was assessed using IC and RhB under visible light irradiation The catalytic process consists of two phases QT1: the dark adsorption equilibrium was established for 60 min QT2: visible-light

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irradiation by A 300 W halogen lamp (Osram, Germany) was used to provide a full spectrum emission without the use of a filter

Chapter 3 RESULTS AND DISCUSSIONS

3.1 ZnBi 2 O 4 /x.0Graphite comsposite

3.1.1 Characterization of ZnBi 2 O 4 /x.0Graphite

Figure 3.1 shows the XRD patterns of graphite, ZnBi2O4 and ZnBi2O4/x.0Graphite The XRD pattern of ZnBi2O4 showed several strong peaks corresponding to tetragonal zinc bismuth oxide and pure hexagonal zinc oxide Pristine graphite typically shows a strong diffraction peak at around 26.6° The diffraction pattern of ZnBi2O4/20.0Graphite was characterized by a new stronger peak at

27.3°as compared to that of pristine ZnBi2O4, indicating hybridization between graphite and ZnBi2O4 The main diffraction peaks of ZnBi2O4/xGraphite were similar to those of ZnBi2O4 and graphite

Figure 3.1 XRD and IR patterns of the samples: ZnBi 2 O 4 and

ZnBi 2 O 4 /xGraphite (x = 1, 2, 5, 10 and 20)

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The ZnBi2O4/x.0Graphite sample exhibited characteristic vibrational peaks at 1480 cm-1 and 1028 cm-1 corresponding to the stretching modes of C=C and C–O groups, respectively The bands at 1384 and

843 cm-1in the pristine ZnBi2O4, ZnBi2O4/x.0Graphitesamples are typically attributed to Bi–O and Bi–O–Bi stretching modes, respectively

The C 1s XPS spectrum of graphite for the ZnBi2O4/1.0Graphite sample is shown in Figure 3.2 A dominant peak at 284.4 eV and a weak peak at 288.1 eV are observed in the graphite spectrum corresponding to C-C (or C=C) and C=O, respectively The binding energies decreasing Zn 2p (0.4 eV), Bi 4f (0.8eV) O 1s (0.3eV) compare the ZnBi2O4/1.0Graphite and ZnBi2O4 sample The strong electronic coupling between ZnBi2O4 and Graphite would likely accelerate the electron-hole separation

Figure 3.2 XPS spectra of ZnBi 2 O 4 and ZnBi 2 O 4 /1.0Graphite

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Figure 3.3 SEM image of

as-prepared samples (a) Graphite,

(b) ZnBi 2 O 4 , and (c-f)

ZnBi 2 O 4 /x.0Graphite (x = 1, 5,

10 and 20); (g) TEM image

ZnBi 2 O 4 /1.0Graphite sample

Figure 3.4 The absorption edges of the samples, and band gap

energy of Graphite, ZnBi 2 O 4 , and ZnBi 2 O 4 /x.0Graphite

The SEM of ZnBi2O4/x.0Graphite samples, ZnBi2O4 tends to grow on the graphite sheet Figure 3.3 shows the typical TEM images of the ZnBi2O4/1.0Graphite composite; it was found that the graphite sheets

were densely covered by the ZnBi2O4 plates

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Bảng 3.1 Band gap energy E g of ZnBi 2 O 4 , Graphit,

(x = 1, 2, 5, 10)

400

535

2.9 2.2 ZnBi2O4/20.0Graphit 420 3.10 The pristine ZnBi2O4 material exhibited visible-light response with the absorption edges at 400 and 535 nm, indicating the presence of a small amount of the ZnO phase, while graphite showed intense absorption over the visible range that extended even to the infrared region (Figure 3.4) The absorption edges of ZnBi2O4/x.0Graphite (x = 1, 2, 5, 10)

were similar to that of ZnBi2O4 and blue-shifted in comparison with those of graphite However, the ZnBi2O4/20.0Graphite composites exhibited a mixed absorption at 420 nm This change indicated a strong interaction between graphite and ZnBi2O4 in the resulting ZnBi2O4/x.0Graphite photocatalysts, which strongly affected the light energy absorption region

3.1.2 Photocatalytic Degradation of IC by ZnBi 2 O 4 /x.0Graphite

Effect of Graphite content in ZnBi 2 O 4 /x.0Graphite composites

The order of the RhB degradation rate for as-prepared photocatalysts was ZnBi2O4/1.0Graphite (0.0141 min–1) > ZnBi2O4/2.0Graphite (0.0077 min–-1) > ZnBi2O4/5.0Graphite (0.0074 min–1) > ZnBi2O4/10.0Graphite (0.0043 min–1) > ZnBi2O4 (0.0032 min–1) > ZnBi2O4/20.0Graphite (0.0018 min–1) The kinetic data of the photodegradation were a good approximation to pseudo-first-order

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kinetic behavior (r 2 = 0.9121–0.9945) The photodegradation rate of

RhB on ZnBi2O4/1.0Graphite was significantly higher (~4.5-fold) than that of ZnBi2O4 Thus, ZnBi2O4/1.0Graphite structure increased the rate of RhB oxidation in comparison with pristine ZnBi2O4 (figure 3.5)

Figure 3.5 Photodegradation of RhB using ZnBi 2 O 4 /xGraphite

catalysts under visible light irradiation

Effect of the loading of ZnBi 2 O 4 /1.0Graphite

When the concentration of ZnBi2O4/1.0Graphite was increased from

0.5 to 1.0 g/L, the rate constant k of RhB degradation increased

significantly from 0.0053 to 0.0141 min–1 (Figure 3.6a) Beyond the ZnBi2O4/1.0Graphite loading of 1.0 g/L, the value of k decreased (0.0137–0.0059 min–1), which may be due to the excessive catalyst causing opacity of the solution, there by hindering light passing through the solution and consequently interfering with the RhB degradation reaction

Effect of initial RhB concentration

The effect of initial RhB concentration on the degradation kinetics was

investigated in range 15–60 mg/mL It can be seen that the rate

constant k of RhB degradation was greatly decreased from 0.0519 to

0.0089 min–1 with the increasing initial RhB concentration from 15 to

60 mg/L This might be explained by the fact that a high concentration

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of RhB lowered the penetration of photons into the solution and this consequently decreased the photodegradation efficiency

Figure 3.6 Photodegradation of RhB over ZnBi 2 O 4 /1.0Graphite under visiblbe light (a) Effect of the loading of ZnBi 2 O 4 /1.0Graphite, (b) Effect of initial RhB concentration, (c) Effect of pH solution, and (d) Reusability of ZnBi 2 O 4 /1.0Graphite catalyst under visible light

Effect of pH solution

Figure 3.6c shows that the maximum degradation of 50 mg/L of RhB over ZnBi2O4/1.0Graphite was more than 93% for a duration of 150 min at pH 2.0 (k = 0.0141), while ~72% and 66% of RhB was degraded

at pH 4.5 (k = 0.0070) and pH 7.0 (k = 0.0059)

Stability and reusability of ZnBi 2 O 4 /1.0Graphit

ZnBi2O4/1.0Graphite exhibited high photochemical stability, even though the photocatalyst had been recycled four times successively

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This implied that the progressive reduction after fourth consecutive cycles was very small Approximately 84.14% of RhB had been successfully degraded after four runs, indicating that the loss in photocatalytic performance of ZnBi2O4/1.0Graphite was insignificant

after four recycling runs

These results indicate that h + and O2 – are the major active species responsible for the complete photocatalytic mineralization of RhB, whereas the contribution of the OH radicals is minor.TOC removal reached 77.7% after visible-light irradiation for 150 min

Figure 3.7 (a) Photodegradation of RhB and (b) The rate constant

k of photodegradation of RhB over ZnBi 2 O 4 /1.0Graphite under visible light with addition of h + ; O 2- and OH radical scavengers and (c) The mechanisms of the RhB photodegradation over

ZnBi 2 O 4 /1.0Graphite under visible light

The enhancement of photocatalytic activity of ZnBi2O4/1.0Graphite

could be mainly attributed to the effective transfer of photogenerated

e- at the heterojunction interface of ZnBi2O4 and graphite, which reduced the recombination of the e- - h+ pairs

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The mechanism for photodegradation of RhB by the ZnBi2O4/1.0Graphite catalyst under visible-light irradiation can be described by the following reactions:

OH + RhB/RhB+  CO2 + H2O

h+ + e–  (e–, h+) (negligible recombination)

3.1.3 Photocatalytic Degradation of IC by ZnBi 2 O 4 /x.0Graphite

The order of the rate constants of the IC decomposition of the catalysts is as follows: ZnBi2O4/5.0Graphite (0.0032 min-1)> ZnBi2O4/2.0Graphite (0.0027 min-1)> ZnBi2O4/1.0Graphit (0.0021 min-1)> ZnBi2O4/10.0Graphit (0.0016 min-1)> ZnBi2O4 (0.0012 min-

1)> ZnBi2O4/20.0Graphit (0, 0007 min-1)

Figure 3.8 Photodegradation of IC over ZnBi 2 O 4 /x.0Graphite (1,

2,5, 10, 20) under visiblbe light

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It can be seen that the ZnBi2O4/1.0Graphite hasn't an good photocatalytic activity for the degradation of RhB under visible light irradiation, on which more than 42,5% of IC had been degraded within

180 min

3.2 ZnBi 2 O 4 /x.0Bi 2 S 3 comsposite

3.2.1 Characterization of ZnBi 2 O 4 /x.0Bi 2 S 3

The XRD pattern of pristine ZnBi2O4 sample is in good accordance with the standard card of tetragonal ZnBi2O4 (JCPDS No 043-0449) and the formation of pure hexagonal ZnO (JCPDS No 079-0207) The main diffraction peaks of ZnBi2O4/x.0Bi2S3 composites were similar to those of the ZnBi2O4 samples However, the patterns

of the ZnBi2O4/x.0Bi2S3 composites showed a low-intensity and wide diffraction peaks, especially the peak at 2 = 28.1, indicating the presence of an amorphous phase after coupling took place between

Bi2S3 and ZnBi2O4

Figure 3.9 XRD and FT- IR patterns of the samples: ZnBi 2 O 4

and ZnBi 2 O 4 /x.0Bi 2 S 3 (x = 1, 2, 6, 12 and 20)

The peak at 3460, 1630 cm-1 in the ZnBi2O4, ZnBi2O4/x.0Bi2S3 spectrum can be referred to OH bonding (FT-IR) The bands at 1384 and

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843 cm -1 in the pristine ZnBi2O4, ZnBi2O4/x.0Bi2S3 samples are typically attributed to Bi–O and Bi–O–Bi stretching modes, respectively The higher the amount of Bi2S3 in ZnBi2O4/x.0 Bi2S3, the more obvious the shift

in the number of Bi-O bonds at the 832 cm-1, proving that there is a chemical interaction that changes the number of characteristic waves

of the bond

Figure 3.10 XPS spectra of ZnBi 2 O 4 and ZnBi 2 O 4 /12.0 Bi 2 S 3

Figure 3.11 UV-Vis spectra, and band gap energy of pristine

ZnBi 2 O 4 , pristine Bi 2 S 3 , and ZnBi 2 O 4/ Bi 2 S 3 composites

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