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The development of digital technology and artificial intelligence technology hastens the progress in the field of digital security. As the latest technology in the field of natural language processing, ChatGPT has become the focus of attention around the world since its birth, and also has a significant impact on the field of digital security. This paper reviews the basic situation of ChatGPT, summarizes and combs the basic concepts of digital security, and then examines and analyzes ChatGPT from the perspective of digital security. It analyzes and sorts out the impact of ChatGPT from six aspects: ChatGPT’s own security, intellectual property security, network security, information security, social security and cognitive security to clarify twenty specific digital security risks. On this basis, the impact of ChatGPT on the fields of equipment intelligence analysis, equipment production and development, and equipment logistics support is analyzed. Finally, this paper provides countermeasures and suggestions from the perspectives of ChatGPT industry development, regulatory construction, false information disposal, and equipment intelligence development.

The effect of coatings (Y2O3, ZrO2 and Al2O3) on the interfacial reaction of TiAl alloys was studied with molecular dynamics. The binding energy of coatings and the diffusion process of oxygen in the melt were simulated, and then the simulation results were compared with the experimental results. The simulation results indicate that for each of the three simulated coatings, inordinate interfacial reactions have occurred between the coating and the melt. The binding energy results show that Y2O3 has the best stability and is the most difficult to break down. ZrO2 has the greatest decomposition energy and is the easiest to break down in the melt. Besides, the molecular dynamics indicate that the diffusion coefficient of the oxygen atom in Al2O3 is larger than that in the other two coatings, indicating that oxygen diffusion in Al2O3 is the fastest at a given temperature. The experimental results show that the oxygen concentration of the melt with Al2O3 coating is the highest, and the oxygen diffusion is of similar magnitude to the simulation values, from which the conclusion can be obtained that the oxygen concentration is significantly influenced by the coating materials. [ABSTRACT FROM AUTHOR]

Whether bis(2-(2′-benzo[4,5-α]thienyl)pyridinato-N,C3′)iridium(acetylacetonate) (btp2Ir(acac)) emission comes from carrier trapping and/or energy transfer, when doped in the 4,4′-bis(N-carbazolyl)biphenyl (CBP) host in organic light-emitting devices, is not clear; therefore, the btp2Ir(acac) emission in CBP hosts was studied. In the red-doped device, both N,N′-bis(1-naphthyl)-N,N′-diphenyl-1.1′-bipheny1-4-4′-diamine (NPB) and (1,1′-biphenyl-4′-oxy)bis(8-hydroxy-2-methylquinolinato)-aluminum (BAlq) emission appeared, which illustrated that CBP excitons cannot be formed at two emissive layer (EML) interfaces in the device. In the co-doped devices, NPB and BAlq emissions disappear and 1,4-bis[2-(3-N-ethylcarbazoryl)vinyl]benzene (BCzVB) emission appears, illustrating the formation of CBP excitons at two EML interfaces in these devices. The reason for this difference was analyzed and it was found that holes in the NPB layer could be made directly into the CBP host in the EML interface of the red-doped device. In contrast, holes were injected into CBP host via the btp2Ir(acac)/BCzVB dopants in the co-doped devices, which facilitated hole injection from the NPB layer to the EML, leading to the formation of CBP excitons at two EML interfaces in the co-doped devices. Therefore, btp2Ir(acac) emission was caused by carrier trapping in the red-doped device, while, in the co-doped devices, it resulted from both carrier trapping and energy transfer from the CBP. Furthermore, it was revealed that the carrier trapping mechanism is less efficient than the energy transfer mechanism for btp2Ir(acac) excitation in co-doped devices. In summary, our results clarified the excitation mechanism of btp2Ir(acac) in the CBP host. [ABSTRACT FROM AUTHOR]

The Eu2+-induced enhancement of defect luminescence of ZnS was studied in this work. While photoluminescence (PL) spectra exhibited 460 nm and 520 nm emissions in both ZnS and ZnS:Eu nanophosphors, different excitation characteristics were shown in their photoluminescence excitation (PLE) spectra. In ZnS nanophosphors, there was no excitation signal in the PLE spectra at the excitation wavelength λex > 337 nm (the bandgap energy 3.68 eV of ZnS); while in ZnS:Eu nanophosphors, two excitation bands appeared that were centered at 365 nm and 410 nm. Compared with ZnS nanophosphors, the 520 nm emission in the PL spectra was relatively enhanced in ZnS:Eu nanophosphors and, furthermore, in ZnS:Eu nanophosphors the 460 nm and 520 nm emissions increased more than 10 times in intensity. The reasons for these differences were analyzed. It is believed that the absorption of Eu2+ intra-ion transition and subsequent energy transfer to sulfur vacancy, led to the relative enhancement of the 520 nm emission in ZnS:Eu nanophosphors. In addition, more importantly, Eu2+ acceptor-bound excitons are formed in ZnS:Eu nanophosphors and their excited levels serve as the intermediate state of electronic relaxation, which decreases non-radiative electronic relaxation and thus increases the intensity of the 460 nm and 520 nm emission dramatically. In summary, the results in this work indicate a new mechanism for the enhancement of defect luminescence of ZnS in Eu2+-doped ZnS nanophosphors. Copyright © 2016 John Wiley & Sons, Ltd. [ABSTRACT FROM AUTHOR]

Whether bis(2-(2'-benzo[4,5-α]thienyl)pyridinato-N,C3')iridium(acetylacetonate) (btp 2 Ir(acac)) emission comes from carrier trapping and/or energy transfer, when doped in the 4,4'-bis(N-carbazolyl)biphenyl (CBP) host in organic light-emitting devices, is not clear; therefore, the btp 2 Ir(acac) emission in CBP hosts was studied. In the red-doped device, both N,N'-bis(1-naphthyl)-N,N'-diphenyl-1.1'-bipheny1-4-4'-diamine (NPB) and (1,1'-biphenyl-4'-oxy)bis(8-hydroxy-2-methylquinolinato)-aluminum (BAlq) emission appeared, which illustrated that CBP excitons cannot be formed at two emissive layer (EML) interfaces in the device. In the co-doped devices, NPB and BAlq emissions disappear and 1,4-bis[2-(3-N-ethylcarbazoryl)vinyl]benzene (BCzVB) emission appears, illustrating the formation of CBP excitons at two EML interfaces in these devices. The reason for this difference was analyzed and it was found that holes in the NPB layer could be made directly into the CBP host in the EML interface of the red-doped device. In contrast, holes were injected into CBP host via the btp 2 Ir(acac)/BCzVB dopants in the co-doped devices, which facilitated hole injection from the NPB layer to the EML, leading to the formation of CBP excitons at two EML interfaces in the co-doped devices. Therefore, btp 2 Ir(acac) emission was caused by carrier trapping in the red-doped device, while, in the co-doped devices, it resulted from both carrier trapping and energy transfer from the CBP. Furthermore, it was revealed that the carrier trapping mechanism is less efficient than the energy transfer mechanism for btp 2 Ir(acac) excitation in co-doped devices. In summary, our results clarified the excitation mechanism of btp 2 Ir(acac) in the CBP host., (Copyright © 2016 John Wiley & Sons, Ltd.)

The Eu 2 + -induced enhancement of defect luminescence of ZnS was studied in this work. While photoluminescence (PL) spectra exhibited 460 nm and 520 nm emissions in both ZnS and ZnS:Eu nanophosphors, different excitation characteristics were shown in their photoluminescence excitation (PLE) spectra. In ZnS nanophosphors, there was no excitation signal in the PLE spectra at the excitation wavelength λ ex  > 337 nm (the bandgap energy 3.68 eV of ZnS); while in ZnS:Eu nanophosphors, two excitation bands appeared that were centered at 365 nm and 410 nm. Compared with ZnS nanophosphors, the 520 nm emission in the PL spectra was relatively enhanced in ZnS:Eu nanophosphors and, furthermore, in ZnS:Eu nanophosphors the 460 nm and 520 nm emissions increased more than 10 times in intensity. The reasons for these differences were analyzed. It is believed that the absorption of Eu 2 + intra-ion transition and subsequent energy transfer to sulfur vacancy, led to the relative enhancement of the 520 nm emission in ZnS:Eu nanophosphors. In addition, more importantly, Eu 2 + acceptor-bound excitons are formed in ZnS:Eu nanophosphors and their excited levels serve as the intermediate state of electronic relaxation, which decreases non-radiative electronic relaxation and thus increases the intensity of the 460 nm and 520 nm emission dramatically. In summary, the results in this work indicate a new mechanism for the enhancement of defect luminescence of ZnS in Eu 2 + -doped ZnS nanophosphors. Copyright © 2016 John Wiley & Sons, Ltd., (Copyright © 2016 John Wiley & Sons, Ltd.)

This study was conducted to investigate the effect of six cryoprotectants (dimethyl sulfoxide (DMSO), glycerol (Gly), methanol (MeOH), ethylene glycol (EG), 1,2-propylene glycol (PG) and N,N-dimethylformamide (DMF) on the survival of medaka (Oryzias lapites) embryos at low temperatures (0 and -5C). Firstly, the embryos at 8 to 16-cell stages were exposed to different concentrations (1 to 4 mol per L) of DMSO, Gly, MeOH, EG, PG and DMF for 40min at 26C. After removal of the cryoprotectants (CPAs), the embryo survivals were assessed by their development into live fries following 9 day of culture. The results showed that the higher concentration of the CPA, the lower survival of the embryos; and that the toxicity of the six CPAs to medaka embryos is in the order of PG < MeOH = DMSO < Gly < EG < DMF (P < 0.05). Secondly, based on the results obtained above, embryos at 8 to 16-cell stages or other stages were exposed to 2 mol per L of PG, MeOH or DMSO for up to 180 min at 0C and up to 80 min at -5C respectively. The 8 to 16-cell embryos treated with MeOH at low temperatures showed highest survival. Thirdly, when embryos at different stages were treated with 2 mol per L of MeOH at -5C for 60 min, 16-somite stage embryos showed highest survival, followed by 4-somite, neurula, 50 percent epiboly, blastula, 32-cell and 8 to 16-cell embryos. These results demonstrated that PG had the lowest toxicity to medaka embryos among the six permeable CPAs at 26C, whereas MeOH showed highest cryoprotective efficiency under chilling conditions and chilling injury decreased gradually with the development of medaka embryos.

This study was conducted to investigate the expression of Histone Deacetyltransferase1 (HDAC1) in mouse embryos derived from the vitrified-warmed oocytes. Firstly, the mouse oocytes at metaphaseII (MII) stage were randomly allocated into three groups: A untreated (control), B exposed to vitrification solution (VS) without being plunged into liquid nitrogen (toxicity), or C vitrified by open-pulled straw (OPS) method (vitrification). After warming, they were fertilized in vitro. Fresh oocytes were used as control. Expression of HDAC1 was then examined in MII mouse oocytes and embryos by immunofluorescence with anti-HDAC1 polyclonal antibody and fluorescein isothiocyanate-conjugated goat anti-rabbit IgG. Results showed that after in vitro fertilization (IVF), developmental rates to two-cell embryos (39%), 4-cell embryos (35%), morula (32%) and blastocysts (26%) in cryopreserved oocytes were all significantly lower than those of fresh oocytes (P < 0.01). In addition, HDAC1 expression in the vitrified group was significantly lower (P< 0.05) than that in the control and toxicity groups at all developmental stages except for the blastocyst. Moreover, the vitrified-warmed oocytes showed significantly lower (P < 0.05) HDAC1 expression compared with that of control and toxicity groups. In conclusion, HDAC1 was expressed both in oocytes and in their in vitro-fertilized embryos. This decreased expression of HDAC1 in mouse oocytes and the embryos due to the cryopreservation may have a negative impact on embryo development.

The present study was designed to investigate the optimized conditions for cryopreservation of Kunming (KM) mice spermatozoa (Experiment 1) and to compare the developmental potential of IVF embryos produced from fresh oocytes (Group 1), vitrified-warmed oocytes without (Group 2) or with partial zona pellucida incised by a piezo manipulator (ZIP) (Group 3) fertilized with frozen-thawed spermatozoa (Experiment 2). In experiment 1, spermatozoa were cryopreserved with the medium containing raffinose and egg yolk with different concentrations (0 to 60 percent) and then followed by fertilization with fresh oocytes after thawing. The highest cleavage (76.2 percent) and blastocysts formation rates (63.6 percent) were obtained when the egg yolk concentration was adjusted to 30 percent. To optimize the equilibration time, the spermatozoa were equilibrated in the optimized medium for 0, 10, 30, 50, 70, 90 min at 40 degree C before plunging into liquid nitrogen. After thawing, the highest cleavage rate (87.4 percent) of IVF embryos was observed when equilibrated for 30 min. In experiment 2, the cleavage and blastocyst rates in Group 1 (81.2 percent, 65.4 percent) and Group 3 (72.5 percent, 45.0 percent) were higher (P less then 0.05) than those in Group 2 (22.2 percent and 13.9 percent), respectively. When 2-cell embryos obtained in Group 1 and 3 were transferred, 32.1 percent and 22.7 percent of embryos in the pregnant receipts developed to term, respectively. In conclusion, the optimized protocol is highly efficient for the cryopreservation of KM mice spermatozoa; the ZIP technique is very useful for improvement of the fertilization efficiency using the cryopreserved gametes and normal offspring can be produced efficiently.