8
Photoluminescence–electricity–magnetism trifunction simultaneously assembled into one flexible nanofiber Shujuan Sheng Qianli Ma Xiangting Dong Nan Lv Jinxian Wang Wensheng Yu Guixia Liu Received: 13 December 2013 / Accepted: 11 January 2014 / Published online: 28 January 2014 Ó Springer Science+Business Media New York 2014 Abstract In order to develop new-typed multifunctional composite nanofibers, Eu(BA) 3 phen/PANI/Fe 3 O 4 /PVP tri- functional composite nanofibers with photoluminescence, electricity and magnetism have been successfully fabricated via electrospinning technology. Polyvinyl pyrrolidone (PVP) is used as a matrix to construct composite nanofibers containing different amounts of Eu(BA) 3 phen, polyaniline (PANI) and magnetite Fe 3 O 4 nanoparticles (NPs). X-ray diffractometry, scanning electron microscopy, transmission electron microscopy, vibrating sample magnetometry, fluo- rescence spectroscopy and Hall effect measurement system are used to characterize the morphology and properties of the obtained composite nanofibers. The results indicate that the trifunctional composite nanofibers possess excellent lumi- nescent, electrical conductivity and magnetic properties. Fluorescence emission peaks of Eu 3? are observed in the Eu(BA) 3 phen/PANI/Fe 3 O 4 /PVP photoluminescent-elec- trical-magnetism trifunctional composite nanofibers and assigned to the of 5 D 0 ? 7 F 0 (580 nm), 5 D 0 ? 7 F 1 (593 nm) of Eu 3? , and the 5 D 0 ? 7 F 2 hypersensitive tran- sition at 615 nm is the predominant emission peak. The electrical conductivity reaches up to the order of 10 -3 S/cm. The luminescent intensity, electrical conductivity and satu- ration magnetization of the composite nanofibers can be tunable by adding various amounts of Eu(BA) 3 phen, PANI and Fe 3 O 4 NPs. The multifunctional composite nanofibers are expected to possess many potential applications in areas such as electromagnetic interference shielding, microwave absorption, molecular electronics and biomedicine. 1 Introduction Electrospinning is an outstanding technique to process viscous solutions or melts into continuous fibers with diameters ranging from micrometer to submicron or nanometer. This method attracts extensive academic investigations, and is also applied in many areas such as filtration [1], optical and chemical sensors [2], biological scaffolds [3] and electrode materials [4]. Europium complexes have excellent luminescent prop- erties owing to the antenna effect of ligands and the f–f electron transition of Eu 3? ions, resulting in important applications in laser, phosphor, and optical data storage devices. However, pure complexes usually do not have good thermal and mechanical stabilities and processing ability, which restrict the complexes to promising extensive photophysical applications and limited practical uses. To overcome these shortcomings, europium complexes usu- ally must be incorporated into organic, inorganic, or organic/inorganic hybrid matrixes, such as zeolites or mesoporous materials [5, 6], sol–gel silica, or organically modified silicates [7] and polymers [8, 9]. Polyaniline (PANI) is one of the most important con- ducting polymers due to its high conductivity, good redox reversibility, processibility, and environmental stability [10, 11] as well as its potential for a variety of applications [11, 12]. In recent years, many one-dimensional (1-D) PANI structures including nanowires, rods and tubes have been studied with the expectation that such materials will combine the advantages of both low-dimensional systems and organic conductors [13]. Sub-micron fibers of pure S. Sheng Á Q. Ma Á X. Dong (&) Á N. Lv Á J. Wang Á W. Yu Á G. Liu Key Laboratory of Applied Chemistry and Nanotechnology at Universities of Jilin Province, Changchun University of Science and Technology, Changchun 130022, China e-mail: [email protected] 123 J Mater Sci: Mater Electron (2014) 25:1309–1316 DOI 10.1007/s10854-014-1728-2

Photoluminescence–electricity–magnetism trifunction simultaneously assembled into one flexible nanofiber

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Photoluminescence–electricity–magnetism trifunctionsimultaneously assembled into one flexible nanofiber

Shujuan Sheng • Qianli Ma • Xiangting Dong •

Nan Lv • Jinxian Wang • Wensheng Yu •

Guixia Liu

Received: 13 December 2013 / Accepted: 11 January 2014 / Published online: 28 January 2014

� Springer Science+Business Media New York 2014

Abstract In order to develop new-typed multifunctional

composite nanofibers, Eu(BA)3phen/PANI/Fe3O4/PVP tri-

functional composite nanofibers with photoluminescence,

electricity and magnetism have been successfully fabricated

via electrospinning technology. Polyvinyl pyrrolidone

(PVP) is used as a matrix to construct composite nanofibers

containing different amounts of Eu(BA)3phen, polyaniline

(PANI) and magnetite Fe3O4 nanoparticles (NPs). X-ray

diffractometry, scanning electron microscopy, transmission

electron microscopy, vibrating sample magnetometry, fluo-

rescence spectroscopy and Hall effect measurement system

are used to characterize the morphology and properties of the

obtained composite nanofibers. The results indicate that the

trifunctional composite nanofibers possess excellent lumi-

nescent, electrical conductivity and magnetic properties.

Fluorescence emission peaks of Eu3? are observed in the

Eu(BA)3phen/PANI/Fe3O4/PVP photoluminescent-elec-

trical-magnetism trifunctional composite nanofibers and

assigned to the of 5D0 ? 7F0 (580 nm), 5D0 ? 7F1

(593 nm) of Eu3?, and the 5D0 ? 7F2 hypersensitive tran-

sition at 615 nm is the predominant emission peak. The

electrical conductivity reaches up to the order of 10-3 S/cm.

The luminescent intensity, electrical conductivity and satu-

ration magnetization of the composite nanofibers can be

tunable by adding various amounts of Eu(BA)3phen, PANI

and Fe3O4 NPs. The multifunctional composite nanofibers

are expected to possess many potential applications in areas

such as electromagnetic interference shielding, microwave

absorption, molecular electronics and biomedicine.

1 Introduction

Electrospinning is an outstanding technique to process

viscous solutions or melts into continuous fibers with

diameters ranging from micrometer to submicron or

nanometer. This method attracts extensive academic

investigations, and is also applied in many areas such as

filtration [1], optical and chemical sensors [2], biological

scaffolds [3] and electrode materials [4].

Europium complexes have excellent luminescent prop-

erties owing to the antenna effect of ligands and the f–f

electron transition of Eu3? ions, resulting in important

applications in laser, phosphor, and optical data storage

devices. However, pure complexes usually do not have

good thermal and mechanical stabilities and processing

ability, which restrict the complexes to promising extensive

photophysical applications and limited practical uses. To

overcome these shortcomings, europium complexes usu-

ally must be incorporated into organic, inorganic, or

organic/inorganic hybrid matrixes, such as zeolites or

mesoporous materials [5, 6], sol–gel silica, or organically

modified silicates [7] and polymers [8, 9].

Polyaniline (PANI) is one of the most important con-

ducting polymers due to its high conductivity, good redox

reversibility, processibility, and environmental stability

[10, 11] as well as its potential for a variety of applications

[11, 12]. In recent years, many one-dimensional (1-D)

PANI structures including nanowires, rods and tubes have

been studied with the expectation that such materials will

combine the advantages of both low-dimensional systems

and organic conductors [13]. Sub-micron fibers of pure

S. Sheng � Q. Ma � X. Dong (&) � N. Lv � J. Wang �W. Yu � G. Liu

Key Laboratory of Applied Chemistry and Nanotechnology at

Universities of Jilin Province, Changchun University of Science

and Technology, Changchun 130022, China

e-mail: [email protected]

123

J Mater Sci: Mater Electron (2014) 25:1309–1316

DOI 10.1007/s10854-014-1728-2

PANI doped with sulfuric acid or hydrochloric acid were

prepared by electrospinning PANI with suitable molecular

weight dissolved in hot sulfuric acid [14]. But it remains a

great challenge to apply electrospinning to PANI as limited

by its molecular weight and solubility. To overcome this

problem, most of the researchers electrospun PANI through

blending it with other spinnable polymers [15, 16].

Magnetic Fe3O4 nanocrystals have been extensively

studied because of its unique and tunable magnetic prop-

erties [17]. Their magnetic features have found widespread

use in applications as diverse as environmental remedia-

tion, magnetic recording, biomacromolecule separation,

catalyst separation, drug/gene delivery and release, and

magnetic resonance imaging [18–21].

In the last few years, multifunctional composite materi-

als have attracted inevasible attention of scientist all over

the world [22, 23]. Some preparations of Fe3O4@RE

complex core–shell structure NPs have been reported [24–

26]. Ma et al. [27, 28] have fabricated Fe3O4/RE complex

(RE = rare earth) magnetic-fluorescent bifunctional com-

posite nanofibers and nanobelts via electrospinning process.

Wang et al. [29] have fabricated PANI particles/rare earth

complex/PVP luminescent-electrical bifunctional compos-

ite nanofibers via electrospinning process. Katal et al. [30]

have prepared Fe3O4/PANI magnetic particles via in situ

emulsion polymerization and discussed its application for

nitrate removal from aqueous solutions. It is found from the

above discussion that multifunction composite materials

have attracted extensive academic research. Presently,

research on multifunction nanomaterials mainly focuses on

the bifunctional nanomaterials, and photoluminescence–

electricity–magnetism trifunction nanofiber has not been

reported in the literatures.

In the present study, we successfully assemble photo-

luminescence-electricity-magnetism trifunction into one

Eu(BA)3phen/PANI/Fe3O4/PVP flexible nanofiber via

electrospinning technique. The photoluminescence-elec-

tricity-magnetism trifunction composite nanomaterial is

expected to apply to the nano device in the future. The kind

of trifunction composite nanofibers can help to reduce the

size of the nano device and are expected to possess many

potential applications in areas such as electromagnetic

interference shielding, microwave absorption, molecular

electronics and biomedicine.

2 Experimental section

2.1 Chemicals

Polyvinyl pyrrolidone (PVP, Mw = 90,000), Eu2O3

(99.99 %), benzoic acid (BA), phenanthroline (phen) and

dimethylformamide (DMF) were bought from Tianjin

Tiantai Fine Chemical Co., Ltd. Anhydrous ethanol, aniline

(ANI), FeCl3�6H2O, FeSO4�7H2O, NH4NO3, polyethyl-

eneglycol (PEG, Mw = 20,000), ammonia and (IS)-(?)-

Camphor-10 sulfonic acid (CSA) were bought from Sin-

opharm Chemical Reagent Co., Ltd. Ammonium persulfate

(APS) were purchased from Guangdong Xilong Chemical

Co., Ltd. All the reagents were of analytical grade and used

directly as received without further purification.

2.2 Preparation of Fe3O4 NPs

Fe3O4 NPs were obtained via a facile coprecipitation

synthetic method, and PEG was used as the protective

agents to prevent the particles from aggregation. One

typical synthetic procedure was as follows: 5.4060 g of

FeCl3�6H2O, 2.7800 g of FeSO4�7H2O, 4.04 g of NH4NO3

and 1.9 g of PEG 20000 were added into 100 ml of

deionized water to form uniform solution under vigorous

stirring at 50 �C. To prevent the oxidation of Fe2?, the

reactive mixture was kept under argon atmosphere. After

the mixture had been bubbled with argon for 30 min,

0.1 mol/L of NH3�H2O was added dropwise into the mix-

ture to adjust the pH value above 11. Then the system was

continuously bubbled with argon for 20 min at 50 �C, and

black precipitates were formed. The precipitates were

collected from the solution by magnetic separation, washed

with deionized water for three times, and then dried in an

electric vacuum oven at 60 �C for 12 h.

2.3 Synthesis of Eu(BA)3phen

Eu(BA)3phen powder were synthesized according to the

traditional method as described in the Ref. [31]. Eu2O3 was

dissolved in an amount of concentrated nitric acid and then

crystallized by evaporation of excess nitric acid and water

by heating, and Eu(NO3)3�6H2O was acquired. Eu(NO3)3

ethanol solution was prepared by adding amount of anhy-

drous ethanol into the above Eu(NO3)3. BA and phen were

dissolved in ethanol in molar ratios of Eu:BA:phen as

1:3:1. The Eu(NO3)3 solution was then added into the

mixture solution of BA and phen with magnetic agitation

for 3 h at 60 �C, and then washed using ethanol for three

times. Finally, the precipitates were collected by filtration

and dried at 60 �C for 12 h.

2.4 Fabrication of photoluminescence-electricity-

magnetism trifunctional composite nanofibers

via electrospinning

In the preparation of spinning solutions, ANI was dissolved

in 4.023 g DMF with magnetic stirring at room tempera-

ture, and then 0.9 g of PVP and CSA were slowly added

into the above solution. The mixture was then cooled down

1310 J Mater Sci: Mater Electron (2014) 25:1309–1316

123

to 0 �C in an ice-bath. The mixture was denoted as solution

I. A mixed solution of APS and 2,000 g of DMF at 0 �C

was prepared as the solution II. The solution II was added

dropwise into the solution I under magnetic stirring. The

final mixture was allowed to react at 0 �C for 24 h and then

Eu(BA)3phen and Fe3O4 were added into the mixture under

magnetic stirring for 12 h at room temperature, thus the

spinning solution was prepared. The dosages of these

materials were shown in Table 1.

During the electrospinning process, a traditional elec-

trospinning apparatus was used to prepare the Eu(BA)3-

phen/PANI/Fe3O4/PVP composite nanofibers. Spinning

solution was loaded into a plastic syringe with a plastic

spinneret, and the inner diameter of the spinneret was

1 mm. A flat iron net was used as a collector and put about

13 cm away from the spinneret. A positive direct current

(DC) voltage of 13 kV was applied between the spinneret

and the collector to generate stable, continuous PVP-based

composite nanofibers under the ambient temperature of

20–25 �C, and the relative humidity was 45–50 %.

2.5 Characterization methods

The as-prepared Fe3O4 NPs and Eu(BA)3phen/PANI/

Fe3O4/PVP composite nanofibers were identified by a X-ray

powder diffractometer (XRD, Bruker, D8 FOCUS) with Cu

Ka radiation. The morphology and internal structure of

Eu(BA)3phen/PANI/Fe3O4/PVP composite nanofibers were

observed by a field emission scanning electron microscope

(FESEM, XL-30) and a transmission electron microscope

(TEM, JEM-2010), respectively. The fluorescent properties

of the Eu(BA)3phen/PANI/Fe3O4/PVP composite nanofi-

bers were investigated by using a Hitachi fluorescence

spectrophotometer F-7000. The elementary compositions of

the Eu(BA)3phen/PANI/Fe3O4/PVP nanofibers were deter-

mined by an energy dispersive spectrometer (EDS,

GENESIE 2000). The conductivity property was detected

by Hall effect measurement system (ECOPIA HMS-3000).

Then, the magnetic performance of Fe3O4 NPs and

Eu(BA)3phen/PANI/Fe3O4/PVP composite nanofibers were

measured by a vibrating sample magnetometer (VSM,

MPMS SQUID XL).All measurements were performed at

room temperature.

3 Results and discussion

3.1 Characterizations of the structure and morphology

X-ray diffractometry patterns of Fe3O4 NPs and composite

nanofibers (S3) are shown in Fig. 1. The XRD patterns in

Fig. 1a reveals that the as-prepared Fe3O4 NPs are con-

formed to the cubic structure of Fe3O4 (PDF 74-0748). No

other characteristic diffraction peaks are detected. XRD

analysis result of the Eu(BA)3phen/PANI/Fe3O4/PVP

composite nanofibers demonstrates that the composite

nanofibers contain Fe3O4 NPs, as shown in Fig. 1b.

In order to characterize the size and shape of the pre-

sented Eu(BA)3phen/PANI/Fe3O4/PVP composite nanofi-

bers, FE-SEM observation is conducted. Figure 2a shows

FE-SEM image of Eu(BA)3phen/PANI/Fe3O4/PVP com-

posite nanofibers, indicating that the as-prepared nanofibers

are relatively smooth. The Image-Pro Plus 6.0 software is

used to measure the diameters of the nanofibers, and the

results are analyzed with statistics. The average diameter

for composite nanofibers is 408 ± 25 nm under the confi-

dence level of 95 %, as indicated in Fig. 3. The TEM

image of Eu(BA)3phen/PANI/Fe3O4/PVP composite

nanofibers (S7) is presented in Fig. 2b. It is obviously seen

from the TEM image that Fe3O4 NPs are well dispersed in

the composite nanofibers. The size distribution of the as-

prepared Fe3O4 NPs is almost uniform, and the diameter of

Table 1 Compositions of the spinning solutions

Compositions ANI/g Fe3O4/g Eu(BA)3

phen/g

CSA/g APS/g

Samples

S1 0.27 0.3 1.08 0.3367 0.6616

S2 0.27 0.3 1.35 0.3367 0.6616

S3 0.27 0.3 1.62 0.3367 0.6616

S4 0.27 0.3 1.89 0.3367 0.6616

S5 0.27 0.3 2.16 0.3367 0.6616

S6 0.27 0.45 1.62 0.3367 0.6616

S7 0.27 0.9 1.62 0.3367 0.6616

S8 0.18 0.3 1.62 0.2245 0.4411

S9 0.36 0.3 1.62 0.4490 0.882120 30 40 50 60 70

2-Theta(degree)

Inte

nsity

(a.u

.)

a

b

PDF#74-0748(Fe3O

4)

Fe3O

4 nanoparticles

Eu(BA)3phen/PANI/Fe

3O

4/PVP

composite nanofibers

Fig. 1 XRD patterns of Fe3O4 NPs and Eu(BA)3phen/PANI/Fe3O4/

PVP composite nanofibers

J Mater Sci: Mater Electron (2014) 25:1309–1316 1311

123

the nanoparticles is 7–10 nm. A slightly agglomeration

phenomenon which can be observed via FE-SEM and TEM

is caused by the large surface energy of the nano-sized

Fe3O4 particles [32]. The EDS analysis, as shown in

Fig. 2c, reveals that the composite nanofibers are consisted

of C, N, O, S, Fe, Eu and Au elements. The Au peak in the

spectrum comes from gold conductive film plated on the

surface of the sample for SEM observation.

3.2 Fluorescent properties of Eu(BA)3phen/PANI/

Fe3O4/PVP composite nanofibers

Figure 4 presents the fluorescent properties of the

Eu(BA)3phen/PANI/Fe3O4/PVP composite nanofibers with

the mass percentages of Eu(BA)3phen to PVP from 120 to

240 %. In order to perform the contrast experiments, the

mass ratios of Fe3O4 to PVP and PANI to PVP are fixed at 1:3

and 30 %, respectively. As indicted in the left part of Fig. 4,

a broad excitation band extending from 200 to 350 nm is

observed when monitoring wavelength is 615 nm. The peak

at 300 nm assigned to the p ? p* electron transition of the

ligands could be also identified. As shown in the right part of

Fig. 4, characteristic emission peaks of Eu3? are observed

under the excitation of 300 nm ultraviolet light and ascribed

to the energy level transitions of 5D0 ? 7F0 (580 nm),5D0 ? 7F1 (593 nm) of Eu3?, and the 5D0 ? 7F2 hyper-

sensitive transition at 615 nm is the predominant emission

peak. For the mass ratios of Eu(BA)3phen to PVP from 120

0 1 2 3 4 5 6 7 8 9 10

c

FeFe

Binding Energy (KeV)

Inte

nsity

(a.

u.)

Eu Eu

s

Au

Au

o

N

c

a

b

Fig. 2 FESEM image (a), TEM image (b) and EDS spectrum (c) of Eu(BA)3phen/PANI/Fe3O4/PVP composite nanofibers

340 360 380 400 420 440 460 480 5000

5

10

15

20

25

30

Diameter (nm)

Per

cent

age

(%)

Fig. 3 Histogram of diameter distribution of Eu(BA)3phen/PANI/

Fe3O4/PVP composite nanofibers

1312 J Mater Sci: Mater Electron (2014) 25:1309–1316

123

to 180 %, the fluorescence intensity of the composite

nanofibers is increased with the increase of addition quan-

tities of Eu(BA)3phen, while the fluorescence intensity

almost remains unchanged after the mass ratio reaches up to

180 %, as shown in Fig. 5.

Besides, in order to study the influence of Fe3O4 NPs on

the fluorescence intensity, the fluorescent emission spectra

(excited by 300 nm) of Eu(BA)3phen/PANI/Fe3O4/PVP

composite nanofibers containing different amounts of

Fe3O4 NPs are indicated in Fig. 6a. From comparing

emission spectrum a to c in Fig. 6a, it is found that the

emission intensity of the composite nanofibers is decreased

with the increase of the amount of Fe3O4 NPs introduced

into the composite nanofibers. This phenomenon can be

explained as the light absorption of Fe3O4 NPs which were

mixed into the nanofibers [33]. From the absorbance

spectrum of Fe3O4 NPs illustrated in Fig. 6b, it is seen that

the Fe3O4 NPs can absorb visible light (400–700 nm) and

much more easily absorb the ultraviolet light (\400 nm).

Thus, the exciting light and emitting light are absorbed by

the Fe3O4 NPs, resulting that the intensities of exciting and

emitting light are decreased. Furthermore, the light

absorption would become stronger with introducing more

Fe3O4 NPs into the composite nanofibers.

Meanwhile, the fluorescent properties of the Eu(BA)3-

phen/PANI/Fe3O4/PVP composite nanofibers with differ-

ent PANI contents are also investigated, as shown in

Fig. 7a. It is clearly observed that emission intensity

decreases with the increase of the PANI content. This

phenomenon can be explained as the light absorption of

PANI which were mixed into the composite nanofibers.

From the absorbance spectrum of PANI illustrated in

Fig. 7b, it is seen that the PANI can absorb UV–Vis light

(300–700 nm) and much more easily absorb ultraviolet

light (300–400 nm) and visible light (600–700 nm). Thus,

the exciting light and emitting light Eu(BA)3phen/PANI/

Fe3O4/PVP composite nanofibers are absorbed by the

PANI, leading to the intensities of exciting light and

emitting light Eu(BA)3phen/PANI/Fe3O4/PVP composite

nanofibers are decreased. Consequently, the light absorp-

tion would become stronger with introducing more PANI

into the composite nanofibers.

3.3 Magnetic property

The magnetic properties of Fe3O4 NPs and Eu(BA)3phen/

PANI/Fe3O4/PVP composite nanofibers are examined by a

vibrating sample magnetometer. No remanence was

detected for the as-prepared Fe3O4 NPs. The zero coer-

civity and the reversible hysteresis behavior indicate the

superparamagnetic nature of the Fe3O4 NPs [34], as

revealed in Fig. 8. The composite nanofibers also demon-

strate superparamagnetism performance owing to Fe3O4

NPs introduced into the composite nanofibers. The varia-

tion of magnetization value is due to different amounts of

Fe3O4 in composite nanofibers. With the increase of Fe3O4

content in composite nanofibers, saturation magnetization

of composite nanofibers increases, as seen in Fig. 8 and

Table 2, which indicates that the magnetic properties of the

composite nanofibers can be tuned via addition of various

amounts of Fe3O4 NPs.

3.4 Electrical conductivity analysis

The average electrical conductivity values of the samples

are summarized in Table 3. The conductivity is greatly

increased from 1.094 9 10-5 to 8.725 9 10-3 S/cm in the

beginning when the PANI is incorporated into composite

nanofibers. With further increase in PANI content, the

200 250 300 350 400 450 500 550 600 650 7000

300

600

900

1200

1500

1800

2100

2400

2700

3000

a

eem = 300 nmem = 615 nm

Inte

nsity

(a.u

.)

Wavelength(nm)

300

580

593

615

e

a

a:Eu(BA)3phen:PVP=120% (S1)

b:Eu(BA)3phen:PVP=150% (S2)

c:Eu(BA)3phen:PVP=180% (S3)

d:Eu(BA)3phen:PVP=210% (S4)

e:Eu(BA)3phen:PVP=240% (S5)

Fig. 4 Excitation spectra (left) and emission spectra (right) of

Eu(BA)3phen/PANI/Fe3O4/PVP composite nanofibers containing dif-

ferent mass percentage of Eu(BA)3phen complex

120 140 160 180 200 220 2401000

1200

1400

1600

1800

2000

2200

2400

2600

2800

Mass percentage (%)

Inte

nsity

(a.

u.)

Fig. 5 Relationship between Eu(BA)3phen contents and intensities of

luminescent peaks at 615 nm for Eu(BA)3phen/PANI/Fe3O4/PVP

composite nanofibers

J Mater Sci: Mater Electron (2014) 25:1309–1316 1313

123

conductivity of composite nanofibers is only slightly

changed. The increase in conductivity of Eu(BA)3phen/

PANI/Fe3O4/PVP composite nanofibers with increasing in

PANI content is due to forming a better continuous net

structure for PANI polymer, and the optimum concentra-

tion of PANI to PVP is 30 %. Furthermore, it is found from

Table 3 that the conductivity of the composite nanofibers is

almost unchanged with increasing in the mass ratios of

300 400 500 600 700 800 900525 550 575 600 625 650 6750

400

800

1200

1600

2000

2400

2800a Fe

3O

4:PVP=1:3(S3)

b Fe3O

4:PVP=1:2(S6)

c Fe3O

4:PVP=1:1(S7)

a

c

580

593

615

Inte

nsity

(a.

u.)

b

ex = 300 nm

a

Wavelength(nm) Wavelength(nm)

Abs

orba

nce(

a.u.

)

Fig. 6 Comparison of emission

spectra of Eu(BA)3phen/PANI/

Fe3O4/PVP composite

nanofibers containing different

mass ratios of Fe3O4 NPs

(a) and UV–Vis absorbance

spectrum of Fe3O4 NPs (b)

300 400 500 600 700 800 900525 550 575 600 625 650 6750

500

1000

1500

2000

2500

3000

3500

580

593

615

c

a

a ANI:PVP=20% (S8)b ANI:PVP=30% (S3)c ANI:PVP=40% (S9)

ex = 300 nm

Wavelength(nm)Wavelength(nm)

Inte

nsity

(a.

u.)

ba

Abs

orba

nce(

a.u.

)

Fig. 7 Comparison of emission

spectra of Eu(BA)3phen/PANI/

Fe3O4/PVP composite

nanofibers containing different

mass percentage of PANI

(a) and UV–Vis absorbance

spectrum of PANI (b)

0-10000 -5000 5000 10000-60

-50

-40

-30

-20

-10

0

10

20

30

40

50

60

a

H(Oe)

M(e

mu

g-1)

d

a:Fe3O

4 nanoparticles

b:Fe3O

4:PVP=1:1

c:Fe3O

4:PVP=1:2

d:Fe3O

4:PVP=1:3

Fig. 8 Hysteresis loops of the a Fe3O4 NPs and Eu(BA)3phen/PANI/

Fe3O4/PVP composite nanofibers containing different mass ratios of

Fe3O4:PVP as b 1:1, c 1:2, and d 1:3

Table 2 Saturation magnetization of Fe3O4 nanoparticles and

Eu(BA)3phen/PANI/Fe3O4/PVP composite nanofibers

Samples Saturation magnetization

(Ms)/emu/g

Fe3O4 nanoparticles 51.40

Fe3O4:PVP = 1:1 (S7) 17.28

Fe3O4:PVP = 1:2 (S6) 10.19

Fe3O4:PVP = 1:3 (S3) 7.07

1314 J Mater Sci: Mater Electron (2014) 25:1309–1316

123

Fe3O4 to PVP when fixing the other parameters, as shown

in samples S3, S6 and S7.

4 Formation mechanism for Eu(BA)3phen/PANI/

Fe3O4/PVP composite nanofibers

We propose the formation mechanism for Eu(BA)3phen/

PANI/Fe3O4/PVP composite nanofibers, as shown in

Fig. 9. Firstly, ANI was dissolved in DMF and PVP to

form solution with some viscosity. Secondly, APS was

mixed above solution and allowed to react at 0 �C for 24 h.

Finally, the prepared Eu(BA)3phen and Fe3O4 NPs were

added into the mixture under magnetic stirring for 12 h at

room temperature, thus the spinning solution was prepared.

The spinning solutions are injected into plastic syringe, and

then Eu(BA)3phen/PANI/Fe3O4/PVP composite nanofibers

are fabricated by electrospinning, as shown in Fig. 9a.

Eu(BA)3phen and Fe3O4 NPs are well dispersed in the

composite nanofibers. PANI also form a continuous net-

work in the nanofibers, leading to a high electrical con-

duction of the photoluminescence-electricity-magnetism

trifunction composite nanofibers, as seen in Fig. 9b.

5 Conclusions

In summary, the photoluminescence-electricity-magnetism

trifunctional composite nanofibers are successfully pre-

pared by electrospinning. The luminescent, conductive and

magnetic intensities of composite nanofibers can be tuned

by adding different concentration of fluorescent material,

PANI and Fe3O4 NPs into them, respectively. The lumi-

nescent intensity of the composite nanofibers is decreased

with the increase of Fe3O4 NPs and PANI content. Magnetic

properties analysis of the composite nanofibers shows that

the saturated magnetization is increased with the increase of

addition quantities of Fe3O4 NPs. These composite nanof-

ibers are shown to be superparamagnetic. The optimum

conductivity of composite nanofibers is 8.725 9 10-3

S/cm. Besides, the design conception and preparation

method of the composite nanofibers are of universal sig-

nificance for the fabrication of other photoluminescent-

electrical-magnetic materials. The new photoluminescence-

electricity-magnetism trifunctional Eu(BA)3phen/PANI/

Fe3O4/PVP composite nanofibers have potential applica-

tions in many fields such as electromagnetic interference

Table 3 Electrical conductivity of the samples doped with various

amount of ANI and Fe3O4

Samples Conductivity

S/cm

Fe3O4:PVP = 1:3

Eu(BA)3phen:PVP = 180 %

ANI:PVP = 20 %

(S8)

1.094 9 10-5

ANI:PVP = 30 %

(S3)

8.725 9 10-3

ANI:PVP = 40 %

(S9)

8.225 9 10-3

Eu(BA)3phen:PVP = 180 %

PANI:PVP = 30 %

Fe3O4:PVP = 1:2

(S6)

5.906 9 10-3

Fe3O4:PVP = 1:1

(S7)

6.784 9 10-3

a b

Fig. 9 Formation mechanism of Eu(BA)3phen/PANI/Fe3O4/PVP composite nanofibers

J Mater Sci: Mater Electron (2014) 25:1309–1316 1315

123

shielding, microwave absorption, molecular electronics and

biomedicine.

Acknowledgments This work was financially supported by the

National Natural Science Foundation of China (NSFC 50972020,

51072026), Ph.D. Programs Foundation of the Ministry of Education

of China (20102216110002,20112216120003), the Science and

Technology Development Planning Project of Jilin Province (Grant

Nos. 20130101001JC, 20070402, 20060504), the Research Project of

Science and Technology of Department of Education of Jilin Province

‘‘11th 5-year plan’’ (Grant Nos. 2010JYT01), Key Research Project of

Science and Technology of Ministry of Education of China (Grant

No. 207026).

References

1. W. Sambaer, M. Zatloukal, D. Kimmer, Chem. Eng. Sci. 66,

613–623 (2011)

2. J.M. Corres, Y.R. Garcia, F.J. Arregui, I.R. Matias, IEEE Sens. J.

11, 2383–2387 (2011)

3. S.A. Sell, P.S. Wolfe, J.J. Ericksen, D.G. Simpson, G.L. Bowlin,

Tissue Eng. Part A 17, 2723–2737 (2011)

4. S.L. Chen, H.Q. Hou, F. Harnisch, S.A. Patil, A.A. Carmona-

Martinez, S. Agarwal, Y.Y. Zhang, S. Sinha-Ray, A.L. Yarin, A.

Greiner, U. Schroder, Energy Environ. Sci. 4, 1417–1421 (2011)

5. M. Alvaro, V. Fornes, S. Garsia, H. Garasia, J.C. Scaiano, J.

Phys. Chem. B 102, 8744–8750 (1998)

6. Q. Xu, L. Li, X. Liu, R. Xu, Chem. Mater. 14, 549–555 (2002)

7. H. Li, S. Inouem, K.-I. Machida, G.-Y. Adachi, Chem. Mater. 11,

3171–3176 (1999)

8. H.-Y. Feng, S.-H. Jian, Y.-P. Wang, Z.-Q. Lei, R.-M.J. Wang,

Appl. Polym. Sci. 68, 1605–1611 (1998)

9. Q. Ling, M. Yang, Z. Wu, X. Zhang, L. Wang, W. Zhang,

Polymer 42, 4605–4610 (2001)

10. D.H. Zhang, Y.Y. Wang, Mater. Sci. Eng., B 134, 9–19 (2006)

11. S. Virji, R.B. Kaner, B.H. Weiller, Chem. Mater. 17, 1256–1260

(2005)

12. Q.H. Zhang, H.F. Jin, X.H. Wang, X.B. Jing, Synth. Met. 123,

481–485 (2001)

13. J. Huang, S. Virji, B.H. Weiller, R.B. Kaner, Chem. Eur. J. 10,

1314–1319 (2004)

14. Q.Z. Yu, M.M. Shi, M. Deng, M. Wang, H.Z. Chen, Mater. Sci.

Eng., B 150, 70–76 (2008)

15. F. Chabert, D.E. Dunstan, G.V. Franks, J. Am. Ceram. Soc. 91,

3138–3146 (2008)

16. J.B. Ballengee, P.N. Pintauro, J. Electrochem. Soc. 158, B568–

B572 (2011)

17. R.M. Cornell, U. Schwertmann, The Iron Oxides, 2nd edn. (VCH,

Weinheim, 2003)

18. D.S. Tang, S.S. Xie, Z.W. Pan, L.F. Sun, Z.Q. Liu, X.P. Zou,

Y.B. Li, L.J. Ci, W. Liu, B.S. Zouand, W.Y. Zhou, Chem. Phys.

Lett. 356, 563–566 (2002)

19. M.C.K. Wiltshire, J.B. Pendry, I.R. Young, D.J. Larkman, D.J.

Gilderdale, J.V. Hajnal, Science 291, 849–851 (2001)

20. P. Trivedi, L. Axe, Environ. Sci. Technol. 34, 2215–2223 (2000)

21. S. Bucak, D.A. Jones, P.E. Laibinis, T.A. Hatton, Biotechnol.

Prog. 19, 477–484 (2003)

22. S.V. Kolotilov, O. Cador, F. Pointillart, S. Golhen, Y.L. Gal, K.S.

Gavrilenko, L. Ouahab, J. Mater. Chem. 20, 9505–9514 (2010)

23. B.K. Balan, V.S. Kale, P.P. Aher, M.V. Shelke, V.K. Pillai, S.

Kurungot, Chem. Commun. 46, 5590–5592 (2010)

24. P. Lu, J.L. Zhang, Y.L. Liu, D.H. Sun, G.X. Liu, G.Y. Hong, J.Z.

Ni, Talanta 83, 450–457 (2010)

25. H.X. Peng, G.X. Liu, X.T. Dong, J.X. Wang, J. Xu, W.S. Yu, J.

Alloys Compd. 509, 6930–6934 (2011)

26. W. Wang, M. Zou, K.Z. Chen, Chem. Commun. 46, 5100–5102

(2010)

27. Q.L. Ma, J.X. Wang, X.T. Dong, W.S. Yu, G.X. Liu, J. Xu, J.

Nanopart. Res. 14, 1–7 (2012)

28. Q.L. Ma, W.S. Yu, X.T. Dong, J.X. Wang, G.X. Liu, Opt. Mater.

35, 526–530 (2013)

29. Y.H. Wang, J.X. Wang, X.T. Dong, W.S. Yu, G.X. Liu, Chem.

J. Chin U 8, 1657–1662 (2012)

30. R. Katal, S. Pourkarimi, E. Bahmani, H.A. Dehkordi, M.A.

Ghayyem, H. Esfandian, J. Vin. Addit. Technol. 51, 5537–5546

(2013)

31. S.B. Meshkova, J. Fluoresc. 10(4), 333–337 (2000)

32. Y.F. Zhu, W.R. Zhao, H.R. Chen, J.L. Shi, J. Phys. Chem. C

111(14), 5281–5285 (2007)

33. Q.L. Ma, J.X. Wang, X.T. Dong, W.S. Yu, G.X. Liu, Chem. Eng.

J. 222, 16–22 (2013)

34. S.H. Xuan, L.Y. Hao, W.Q. Jiang, X.L. Gong, Y. Hu, Z.Y.J.

Chen, Magn. Magn. Mater. 308, 210–213 (2007)

1316 J Mater Sci: Mater Electron (2014) 25:1309–1316

123