No | Name | Rank | Photo | |
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1. | Dr. Than Than Lwin | Professor & Head | thanthanlwin@bmwuni.edu.mm | |
2. | Dr. U Thaung Yee | Professor | thaungyi@bmwuni.edu.mm | |
3. | Dr. Hla Hla Win | Associate Professor | hlahlawinphys@bmwuni.edu.mm | |
4. | Dr. Zin Zin Naing | Associate Professor | zinzinnaing@bmwuni.edu.mm | |
5. | Dr. Khin Htwe | Associate Professor | khinhtwe@bmwuni.edu.mm | |
6. | Dr. Maung Maung Soe | Associate Professor | mgmgsoe@bmwuni.edu.mm | |
7. | Dr. Khaing Po Po | Lecturer | khaingpopo@bmwuni.edu.mm | |
8. | Dr. Aye Myat Wai | Lecturer | ayemyatwai@bmwuni.edu.mm | |
9. | Daw Hlaing Hlaing Maw | Lecturer | hhmaw@bmwuni.edu.mm | |
10. | Dr. Thidar Aung | Lecturer | thidaraung@bmwuni.edu.mm | |
11. | Dr. Lae Lae Win Hlaing | Lecturer | lailai@bmwuni.edu.mm | |
12. | Dr. San San Htwe | Lecturer | sansanhtwe@bmwuni.edu.mm | |
13. | U Thet Naing Myo | Lecturer | thetnaingmyo@bmwuni.edu.mm | |
14. | U Bawk Lar | Lecturer | bawkla@bmwuni.edu.mm | |
15. | Daw Sandar Soe | Assistant Lecturer | sandarsoe@bmwuni.edu.mm | |
16. | Daw May Zin Nyein | Demostrator | mayzinnyein@bmwuni.edu.mm |
No | AUTHOR | Research Name | Abstract | Journal Name, Vol.Name, Date | ||
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1 | Dr Hla Hla Win | ΛΛ − ΞN Coupling Effect in LL5H System | The purpose of our research is to investigate - interaction energy and the coupling effect in the double strangeness five-body hypernuclear system within the framework of three-body coupled-channel Gaussian basis treatment. We have solved two-coupled-channel three-body Schrödinger equation for various baryon-baryon potential models; NHC-D, NSC 97e and NHC-F in strangeness S= -2 sector. Our calculated interaction energy between two , ( ), for system by using coupled-channel are 1.07 MeV, 0.40 MeV and 0.04 MeV for NHC-D, NSC 97e and NHC-F respectively. By applying the coupled-channel formalism, the coupling effects are found to be 0.02 MeV, 0.05 MeV and 0.05 MeV for NHC-D, NSC 97e and NHC-F respectively. It is found that the coupling effect in NHC-F is the largest, since coupling strength of NHC-F is the strongest. mixing in ground state are found to be 0.02 % , 0.05 % and 0.06 % for NHC-D, NSC 97e and NHC-F respectively. It indicates that the coupling potential between the and channels is rather weak. Thus it is concluded that system is an almost pure LL state with a very small component. | Banmaw University Research Journal, 2011 December, Vol.4, No.4(Pg 117-129) | ||
2 | Dr Hla Hla Win | Resonance States of α−n System by Applying Complex Scaling Method | The purpose of this research is to study the resonance energy of (_2^5)He (, n) system by solving the two body Schrödinger equation with complex scaling method. The Gaussian basis wave function is used to solve the two body Schrödinger equation for (J = 3/2- ) state and (J = 1/2- ) state in spin-orbit coupling. The calculated resonance energies and level widths for (J = 3/2- ) state and (J = 1/2- ) state are (0.747, 0.596) MeV and (2.147, 5.533) MeV respectively. Comparison is made with the experimental data and good agreement is found. | Journal of the Myanmar Academy of Arts and Science, 2018 October, Vol.XVI, No.2(Pg 105-117) | ||
3 | Dr Hla Hla Win | ΛΛ Interaction Energies in LL5H System | The purpose of this research is to investigate - interaction energies in the double strangeness five-body hypernuclear system within the framework of three-body Gaussian basis treatment. Due to the lack of Λ-Λ scattering data, double Λ-hypernuclei provide a unique method to learn details on the Λ-Λ interactions. We have solved the three-body Schrödinger equation for various baryon-baryon potential models; NHC-D, NSC 97e and NHC-F in strangeness S= 2 sector. Our calculated interaction energies between two , ( ), for system are 1.05MeV, 0.35MeV and -0.01MeVfor NHC-D, NSC 97e and NHC-F respectively. Keywords: rearrangement coupled channel method, - interaction energy. | Banmaw University Research Journal, 2018 August, Vol.10, No.11(Pg 135-144) | ||
4 | Dr Hla Hla Win | ΛΛ − ΞN Coupling Effect on Λ−Λ Interaction Energy in LL5H System | Proceeding of the International Conference on Physics, Mandalay (ICPM 2018), 2018 November | |||
5 | Dr Hla Hla Win | Three Body Calculation of LL5H System | The purpose of this research is to investigate the binding energy of double strangeness five-body hypernuclear system within the framework of three-body Gaussian basis treatment. We have solved the three-body Schrödinger equation for various baryon-baryon potential models; NHC-D, NSC 97e and NHC-F in strangeness S= 2 sector. The calculated binding energies of system in NHC-D, NSC 97e and NHC-F models are 3.59 MeV, 2.89 MeV and 2.53 MeV respectively for single channel. The calculated interaction energy between two , ( ), for system are 1.05MeV, 0.35MeV and -0.01MeVfor NHC-D, NSC 97e and NHC-F respectively. From our calculation, we found that binding energies of in NHC-D are the largest because this model has the strongest interaction potential among the three models. | Mandalay University Research Journal, 2018 December, Vol.9, No.2(Pg 108-112) | ||
6 | Dr Hla Hla Win | Structure Calculation of L5He Two-body System | The purpose of this research is to investigate the structure of System. We have considered the hypernucleus as two body system with one particle and one particle. In this work, we have used Dalitz-Down ( DD ) and Tang-Herndon ( TH ) - potentials. We have calculated norm matrix element Nij, kinetic energy matrix element Tij and potential energy matrix element Vij by analytically. Then we have carried out the binding energy of hypernucleus system by using these matrix elements with FORTRAN CODE. The calculated average kinetic energy of hypernucleus for ( DD ) and ( TH ) potentials are 9.15MeV and 11.25MeV. The average potential energy of hypernucleus are -12.24MeV and -14.29MeV for ( DD ) and ( TH ) potentials respectively. The root-mean square distance of hypernucleus are 2.76fm and 2.62fm for ( DD ) and ( TH ) potentials respectively. Our calculated binding energies of hypernucleus system are 3.09MeVand 3.04MeV with ( DD ) and ( TH ) potentials respectively. The experimental binding energy of hypernucleus system is 3.12±0.02 MeV. Our calculated binding energies of are nearly consistent with the experimental data. | Taunggyi University Research Journal, 2019 June, Vol.10, No.2(Pg 109-112) | ||
7 | Dr Hla Hla Win | The Neutron Single Particle Energy Levels in 50114Sn Nucleus | The purpose of our research is to investigate the neutron single particle energy levels of (_50^114)Sn nuclei by assuming that a nucleon moves independently in an averaged potential well. The radial Schrödinger equation is solved numerically by using Numerov method. It is found that the calculated neutron single particle energy levels of (_50^114)Sn nucleus for Harmonic Oscillator potential are consistent with the analytical results. | Engineering Technology and Science Journal (ETSJ), 2019, Vol.1, Issue.1(Pg 414-420) | ||
8 | Dr Hla Hla Win | Two-body Calculation of L5He System with MSA Potential | The purpose of this research is to investigate the structure of single strangeness hypernuclear system within the framework of two-body Gaussian basis treatment. We have solved the two-body Schrödinger equation for Myint, Shinmura and Akaishi (MSA) - potential. We have investigated the average kinetic energy (KE), average potential energy (PE), the binding energy (BE ) and root-mean-square distance (Rms) for system. The calculated average kinetic energy and average potential energy of system are 6.23 MeV and -9.36 MeV. The root-mean square distance of system in MSA model is 1.56 fm. The calculated binding energy of hypernucleus system is 3.13 MeV. The experimental binding energy of hypernucleus is (3.12±0.02) MeV. It is found that our calculated binding energy of system is consistent with experimental value. | Research Paper Reading Seminar in Commemoration of the 23rd Anniversary of Monywa University, 2019 October, Proceeding(Pg 80-84) | ||
9 | Dr Hla Hla Win | Structure Calculation of LL5H System | The purpose of this research is to investigate the structure of the double strangeness five-body hypernuclear system within the framework of three-body Gaussian basis treatment. The three-body Schrödinger equation are solved for various baryon-baryon potential models; NHC-D, NSC 97e and NHC-F in strangeness S= 2 sector. The calculated binding energies of in NHC-D, NSC 97e and NHC-F models are 3.59 MeV, 2.89 MeV and 2.53 MeV respectively for single channel. The binding energies of this system is increased to 3.63 MeV, 2.99 MeV and 2.65 MeV for above mention potentials when the coupling effect is included. The pauli forbidden state between the triton and converted particle proton is considered. The calculated binding energies for system with Pauli suppression effect are 3.61 MeV, 2.94 MeV and 2.58 MeV for NHC-D, NSC 97e and NHC-F respectively. It is observed that the binding energies of system in NHC-D are the largest because this model has the strongest interaction potential among the three models. | Banmaw University Research Journal, 2019 August, Vol.11, No.2(Pg 101-110) | ||
10 | Dr Hla Hla Win | The L-single Particle Energy Levels in L16O Hypernucleus | The purpose of this research is to investigate single particle energy levels of hyper-nucleus by assuming that single moves independently in an averaged potential well which has the Woods-Saxon form including spin-orbit interaction. The radial Schrödinger equation is solved numerically by using Numerov Method. The calculated results are compared with other theoretical results. The calculated results of Ʌ single particle energy levels of hyper-nucleus are in good agreement with other theoretical result. | Banmaw University Research Journal, 2020 June,Vol.11, No.1(Pg 169-175) | ||
11 | Dr Hla Hla Win | Energy and Level Width of 25He ( Jp=3/2- ) System | The purpose of this research is to investigate the energy and level width of system. The Gaussian basis wave function is used to solve the two body Schrödinger equation with spin-orbit coupling. The calculated resonance energy and level width is compared with the experimental data and good agreement is found. | Banmaw University Research Journal, 2020 June,Vol.11, No.2(Pg 148-153) | ||
12 | Dr Hla Hla Win | Structure Calculation of h16O Nucleus | The purpose of this research is to investigate the structure of -mesic oxygen nucleus theoretically which is a bound system of -meson and Oxygen core nucleus. Since original functional form of η-N interaction cannot be analytically solved, we have transformed the functional form into Gaussian form by applying the Gauss elimination method. The transformed η-N potentials are equivalent to that of original potential by using the optimum sets, and N=20. The η-nucleus interaction is obtained by folding the η-N interaction with Oxygen nucleus nuclear density. By applying the η-nucleus folding potential we have computed the binding energy of system which is 3.2814 MeV and its level width is 0.3704 MeV. | Journal of the Myanmar Academy of Arts and Science, 2020 July,Vol. XVIII, No.2C(Pg 37-46) | ||
13 | Dr Maung Maung Soe | Microcontroller Based Water Tap Control System | The microcontroller based water tap control system is designed and constructed using ultrasonic sensors, PIC microcontroller, DC motor, motor driver circuit, amplifiers circuits and other electronic components. A pair of ultrasonic sensors (transmitter and receiver) is the main part of the system to detect an existence of an object under the water tap. The ultrasonic sensors are mounted side by side over the water tap and pointed to the downward direction. The ultrasonic transmitter circuit sends the ultrasonic wave. The ultrasonic receiver circuit accepts that signal as an echo when an object enters a predefined place. The microcontroller sends control signals to the motor drive circuit when it receives object detect signals from the ultrasonic receiver circuit. The DC motor is applied to turn the water tap. The range of ultrasonic detection is set to detect an object up to about 30 cm from the sensors. The constructed system can be used to open automatically the water tap of the basin when the hand or any other objects is put under the tap. | Banmaw University Research Journal, 2020 June, Vol.11, No.2(Pg 162-169) | ||
14 | Dr Maung Maung Soe | Design and Construction of Stroboscope Based on PIC Microcontroller | The stroboscope using the electronic strobe method for the measurement of frequency for a rotating object is designed and constructed. The constructed stroboscope mainly consists of PIC 16F887 microcontroller, 16 x 2 line liquid crystal display (LCD) module, high power super bright LED, 555 timer circuit and other electronic components. The frequency and PWM (pulse width modulation) of the circuits are controlled by using two variable resistors. The signal output is sent to the LED driver circuit as well as the microcontroller circuit. The super bright LED produces flashing light corresponding to the generated frequency and PWM. The microcontroller counts the frequency of the signal and displays the frequency in hertz (Hz) and revolution per minute (RPM) units on the LCD module. The flashing LED is pointed to the rotating object whose speed is to be measured. The frequency and PWM are adjusted until the still image of the rotating object is obtained. The stroboscope is designed to measure the RPM of the object from 240 to 1500 RPM. The constructed LED stroboscope can measure the speed of the rotating object from the distance of up to 2 m using non-contact method. | Banmaw University Research Journal, 2020 June, Vol.11, No.2(Pg 162-169) | ||
15 | Dr Maung Maung Soe | PC-Based Temperature and Radiation Monitoring System | The PC-based temperature and radiation monitoring system is constructed. The temperature sensor circuit is constructed by using silicon semiconductor temperature sensor KTY81-121. The small pocket size Geiger-Muller counter K2645 is used for radiation detection. The readings of temperature and radiation dose-rate are displayed on the 16 x 2 line liquid crystal display (LCD) module. The ATMega 8 microcontroller is used to control the operations of the system. The data transfer between microcontroller and PC is done via EMANT 300 USB data acquisition (DAQ) module. The measured temperature and radiation values are also displayed on the monitor of the PC. The graphical programming software, LabVIEW is used to handle data and to display messages on the monitor. | Banmaw University Research Journal, 2009 December,Vol.2, No.3(Pg 27-39) | ||
16 | Dr Maung Maung Soe | Microcontroller-base sine Wave and Square Wave Signal Generator | The microcontroller – based sine wave and square wave signal generator is designed and implemented using ATMega 8 microcontroller, 8-bit digital-to-analog converter and other electronic components. The signal generator can generate sine wave and square wave signals from the frequency of about 1 Hz to about one hundred kilo hertz range with user selectable frequency. The wave form selector switch enables the user to choose either the sine wave or the square wave to be generated. The potentiometer can be used to adjust the frequency of the generated signal. | Banmaw University Research Journal, 2010 December, Vol.3, No.3 (Pg 127-136) |
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17 | Dr Maung Maung Soe | Design and Implementation of chip KIT Uno 32 Based GM Counter | The portable GM counter is designed and implemented using chipKIT Uno32 microcontroller board and the Velleman’s K2645 Geiger Muller (GM) counter module. The GM counter module consists of the GM tube and DC high voltage circuit. The radiation coming into the GM tube produces a small current due to the flow of electrons and positive ions. The electrons are then accelerated using high voltage to produce a small current pulse at the anode of the GM tube. The voltage pulse is obtained by placing appropriate resistor at the output. The output voltage pulse is used to drive the buzzer. The buzzer makes the sound every time the radiation enters the GM tube. The output voltage pulse has a peak of about 9 V. The voltage pulse is then divided using series resistors to obtain one third of the original value. The pulse is then fed to the input of the chipKIT Uno32 board to count the radiation. The radiation doses in μR/h are displayed on the LCD module. | University of Mandalay Research Journal, 2015 December,Vol.6, No.1(Pg 113-120) | ||
18 | Dr Maung Maung Soe | Implementation of 74F381 ALU Function using Altera. Cyclone IV FPGA Board | The functions of the arithmetic logic unit (ALU) IC, 74F381 is implemented using Altera’s Cyclone IV field programmable gate array (FPGA) board. The ALU is an essential part of the microprocessors and microcontrollers. The ALU is mainly used to do arithmetic operations such as addition, subtraction, division and multiplication and logic operations such as AND, OR, NOT, NAND and NOR. The implement ALU performs three arithmetic and three logic operations on two 4-bit words, A and B. The ALU also has three function select inputs, S0-S2 and four outputs, F0-F3 as well as the carry input, Cn, the carry propagate output,( P) ̅, and carry generate output, G ̅ . The FPGA board is programmed by using VHDL (Very high speed integrated circuit Hardware Description Language) language. The peripheral circuits such as switch input circuit (data input circuit) and LED display circuit (data output circuit) are constructed to test the ALU function. Finally, the constructed board is tested by giving various input combinations (arithmetic and logic functions) and observing the outputs and then compares with the 74F381 ALU IC. | University of Mandalay Research Journal, 2016 December,Vol.7, No.1(Pg 149-156) | ||
19 | Dr Maung Maung Soe | Design and Implementation of UV Index Monitoring System Based on UV Sensor, Bluetooth and Lab VIEW | The UV index monitoring system is designed and constructed. The constructed system can be divided into two separate parts: UV index measuring section and UV index measuring system. The constructed system mainly consists of PIC16F887 microcontroller, 16 x 2 line LCD module, GUVA-S12SD UV sensor module, HC-06 Bluetooth module and LM7805 voltage regulator. The UV sensor measures and monitors UV radiation from the sun. The output of the sensor is sent to the PIC 16F887 microcontroller. The analog voltage received from the sensor is converted into digital data format inside the microcontroller. The digital data is processed inside the microcontroller to obtain the UV index reading. Then the data is sent to the LCD module to display the UV index reading. At the same time, the data is converted into serial data format and sends to the input of the Bluetooth module. The data transfer between microcontroller and PC is done via Bluetooth module. The measured UV index values are also displayed on the monitor of the PC. The graphical programming software, LabVIEW is used to handle data and to display messages on the monitor. | University of Mandalay Research Journal, 2017 December,Vol.8, No.1(Pg 350-359) | ||
20 | Dr Maung Maung Soe | Design and Construction of FPGA Based Training Board for Digital Electronics Experiments | The training board for Digital Electronics experiments is constructed by using Altera’s Cyclone FPGA and other supported electronic components. The core FPGA board based on Cyclone IV FPGA is used as the main control unit. The FPGA board is programmed by using VHDL (Very high speed integrated circuit Hardware Description Language) language. The peripheral circuits (such as switch input circuit, LED display circuit, 7-segment LED display) are also constructed to test the function of the FPGA and VHDL language. Finally, the constructed training board is tested by writing various programs and downloading the file into the FPGA board. The constructed board can be used to do the basic Digital Electronics experiments for the students, especially for the Post Graduate students specialized in Electronics (Physics). Keywords: FPGA, VHDL | Proceeding of the International Conference on Physics, Mandalay (ICPM 2018), 2018 November(Pg 413-417) | ||
21 | Dr Zin Zin Naing | Automation Using Bluetooth, Android And Arduino | The electrical appliances can be controlled by android smart phone from the remote location (within 30ft in diameter). Bluetooth, android smart phone and Arduino microcontroller are used in this home automation system. Bluetooth device HC-05 is connected to the Arduino. And then, it is paired to the android phone via Bluetooth technology. Bluetooth HC-05 receives the message sent from android phone and sends to Arduino microcontroller. As soon as the main processing unit, Arduino, receives the information from Bluetooth, it makes the processing to control the home appliances “ON “or “OFF”. EEPROM is used to store the relay’s final status when the power is in failure so that system is operated in last memory status when the power has come up. | Banmaw University Research Journal, 2020 June,Vol.11, No.2(Pg 170-177) | ||
22 | Dr Zin Zin Naing | Real Time Physical Data Logger | The data of temperature which is the output of LM 35 sensor are detected by the Arduino. At the same time, the current time can be interpreted by real time clock (RTC 1307 IC). Temperature with real time clock can be expressed on the serial monitor and can be stored in the SD card. Arduino Uno, data logger breakout, real time clock and LM 35 temperature sensor are used in logging the temperature with real time. | Banmaw University Research Journal, 2020 June,Vol.11, No.2(Pg 178-183) |
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23 | Dr Zin Zin Naing | Data Acquisition of Solar Radiation and Ultra-Violet ( UV ) Intensity | The intensity of solar radiation and UV radiation are measured using BH1750 by BH1750 sensor and light sensor and ML 8511 UV sensor respectively. The process is implemented by using microcontroller. As BH 1750 light sensor is inter- integrated circuit (I2C) device, it is connected to microcontroller with I2C mode. The data from each sensor are sent to Arduino microcontroller and then, data are displayed on LCD. Simultaneously, the intensity of light and UV radiation are logged in excel spreadsheet directly using the parallex data acquisition (PLX-DAQ) software. These data are uploaded directly to Microsoft (MS) excel spreadsheet directly with the accompanying the current date and time. | Journal of the Myanmar Academy of Arts and Science, 2020 July,Vol. XVIII, No.2B(Pg 383-390) | ||
24 | Dr Zin Zin Naing | Characterization of Lead Bismuth Cuprous Glasses | Journal of the Myanmar Academy of Arts And Science, 2009 March,Vol-XII No-2B(Pg 1-10) | |||
25 | Dr Zin Zin Naing | Arduino Embedded Ambient Humidity and Temperature Controlled System | Taungoo University Research Journal, 2014 February,Vol-V No-1(Pg 115-124) | |||
26 | Dr Zin Zin Naing | Design and Analysis of Frequency Generator Using Proteus Software | The frequency generator circuits are designed by using the different microcontrollers which consist of capture, compare and pulse width modulation module (CCP). Using the Basic Pro language and microC language, frequency is changed by various steps. The proposal design is drawn by ISIS software and it is checked by interactive simulation with the help of Proteus software. The desired output frequency can be changed by ±1Hz, ±10Hz, ±100Hz, ±1000Hz steps or the specified frequency can be obtained by pressing input switches. The variations of the initial output frequency and the maximum output frequency are observed by using the different crystal oscillators and the different microcontrollers. | Journal of the Myanmar Academy of Arts And Science, 2014 March,Vol-XII No-2(Pg 343-353) | ||
27 | Dr Zin Zin Naing | GSM Based Fire Alarm System | GSM based fire alarm system is designed to send SMS to the specified mobile phones when the temperature is higher than the critical temperature due to the fire. The Arduino Uno R3 is a microcontroller board based on the ATmega328. The Arduino SIM 900 GSM Shield is allowed to easily connect the Arduino to the GSM network. This shield enables Arduino to send SMS anywhere in the world with an internet connection. The Arduino software serial library is used, and this shield has wired the serial from the SIM900 to a set of jumpers, and uses a default speed of 9600. Sketch is written by ArduinoC. DS 18B20 temperature sensor is used to monitor the environment temperature. If the temperature is above the critical temperature, Arduino commands the GSM shield to send the SMS messages to the specified GSM phones. | Taungoo University Research Journal, 2017 March, Vol-VIII No-1(Pg 43-49) | ||
28 | Dr Zin Zin Naing | Data Acquisition of Solar Insolation Using PLX-DAQ Software | The intensity of solar radiation and UV radiation are measured using BH1750 by BH1750 sensor and light sensor and ML 8511 UV sensor respectively. The process is implemented by using microcontroller. As BH 1750 light sensor is inter- integrated circuit (I2C) device, it is connected to microcontroller with I2C mode. The data from each sensor are sent to Arduino microcontroller and then, data are displayed on LCD. Simultaneously, the intensity of light and UV radiation are logged in excel spreadsheet directly using the parallex data acquisition (PLX-DAQ) software. These data are uploaded directly to Microsoft (MS) excel spreadsheet directly with the accompanying the current date and time. | Taungoo University Research Journal, 2019 July,Vol-10 No-1(Pg 176-180) | ||
29 | Dr Aye Myat Wai | Calculation of Heavy-Ion Fusion Cross Sections Using Different Nuclear Potentials | The fusion cross sections and fusion barrier distributions of 16O + 148,154Sm systems have been calculated using different types of nuclear potentials. Simple one-dimensional potential model and coupled-channels method have been applied. The calculated results are compared with the experimental data. The calculated fusion cross sections using one-dimensional potential model disagree with the experimental data. The improvements have been made by inclusion of channel coupling effects. The calculated fusion cross sections are also analyzed by calculating the fusion barrier distributions which is sensitive to details structure of the colliding nuclei. | Journal of the Myanmar Academy of Arts and Science, 2020 July,Vol. XVIII, No.2B(Pg 319-325) | ||
30 | Dr Aye Myat Wai | Coupled-Channels Calculations of Fusion Cross Sections and Fusion Barrier Distributions for 32,36S + 90Zr Systems | The fusion cross sections and fusion barrier distributions of 32,36S + 90Zr systems have been calculated using Woods-Saxon nuclear potentials. Coupled-channels method and the code CCFULL are used in the calculations. The calculated results are compared with the experimental data. From the results, the information of the nuclei such as the types of coupling, multipolarity and number of phonons for the reactions can be obtained. | Banmaw University Research Journal, 2020 June,Vol.11, No.2(Pg 184-189) | ||
31 | Dr Aye Myat Wai | Coupled-Channels Calculations of Heavy-Ion Fusion Reactions | The fusion cross sections and fusion barrier distributions of 16O + 148,154Sm systems have been calculated using different types of nuclear potentials. Simple one-dimensional potential model and coupled-channels method have been applied. The calculated results are compared with the experimental data. The calculated fusion cross sections using one-dimensional potential model disagree with the experimental data. The improvements have been made by inclusion of channel coupling effects. The calculated fusion cross sections are also analyzed by calculating the fusion barrier distributions which is sensitive to details structure of the colliding nuclei. | Banmaw University Research Journal, 2017 August,Vol. 9, No.4(Pg 23-27) | ||
32 | Dr San San Htwe | Study on Gamow-Teller Transition Strengths In Beta Decay of 24 Al | The Gamow-Teller transitions of 24Al through nuclear beta-decay were studied. The beta-decay processes are also investigated. The beta-decay probability of the nucleus is calculated using time-dependent perturbation theory. The relation between the beta-decay probability and the comparative half-life of beta emitter were derived. By using this relation, the transition strengths of 24Si, beta-plus (β+) decay of 24Al, are calculated. Finally, our results were compared with those from other research paper. | Banmaw University Research Journal, 2020 June, Viol.11, No.2(Pg 202-206) | ||
33 | Dr Lai Lai Win Hlaing | Investigation of Phase Formation and Structural Properties of LiCo(1-x) Nix O2 | Banmaw University Research Journal, 2020 June, Viol.11, No.2(Pg 190-201) |
No. | Candidate | Thesis Title | Supervisor | Year | |
---|---|---|---|---|---|
1. | Ma Phyu Hnin Phway | Construction of Radio Frequency Identification (RFID) Based Attendance System Using Arduino | Dr. Khin Htwe Associate Professor | 2020 | |
2. | Ma May Thu Zar Win | Construction of Vehicle Speed Detector Using Arduino | Dr. Khin Htwe Associate Professor | 2020 | |
3. | Ma Zahkung Hkawn Htoi Aung | Design and Construction of Soil Moisture Monitoring System | Dr. Maung Maung Soe Associate Professor | 2020 | |
4. | Ma Aye Aye Chit Moe | Design and Construction of Water Level Control System | Dr. Maung Maung Soe Associate Professor | 2020 | |
5. | Ma Mya Sabae Hpoo | Design and Construction of Arithmetic Logic Unit (ALU) Based on PIC Microcontroller | Dr. Maung Maung Soe Associate Professor | 2020 | |
6. | Ma Lum Seng Pan | Design and Construction of Microcontroller Based Digital Logic Training Board | Dr. Maung Maung Soe Associate Professor | 2020 | |
7. | Ma Lahpai Nem Ja | Data Acquisition of Mini-weather Station Using PLX-DAQ Software | Dr. Zin Zin Naing Associate Professor | 2020 | |
8. | Ma Lu Lu San | Internet of Thing (IOT) Based Data Acquisition by Using Thingspeak Server | Dr. Zin Zin Naing Associate Professor | 2020 | |
9. | Ma Tin Zar Lae | A Study on Structural Properties of Manganese Bismuth Borate Glasses | Dr. Khaing Po Po Lecturer | 2020 | |
10. | Ma Shwe Zin Htoo | Calculation of Transmission Probabilities Depend on Barrier Height and Barrier Width for Incident Electron | Dr. Aye Myat Wai | 2020 | |
11. | Ma Nan Shwe Yin | Construction of PIC Based Three Digit Counter Using Seven Segment Display | Daw Hlaing Hlaing Maw Lecturer | 2020 | |
12. | Ma Ei San Phyo | Design and Construction of Microcontroller Based Running Light Display | Dr. Thida Aung Lecturer | 2020 | |
13. | Ma Ja Sim Pan | Synthesis and XRD Studies of Nickel Doped Lithium Cobalt Oxide | Dr. Lai Lai Win Hlaing Lecturer | 2020 | |
14. | Ma Yee Yee Htay | Calculation of Ground State Energies for Some Helium like Atoms | Dr. San San Htwe Lecturer | 2020 | |
15. | Ma Ei Thae Phyo | Design and Construction of Andriod Phone Controlled Electrical Devices | U Thet Naing Myo Lecturer | 2020 | |
16. | Ma Pausa Seng Num | Microcontroller Based Automatic Door and Room Light Control System | U Bawk La Lecturer | 2020 | |
17. | Ma Khine Khine Moe | Microcontroller Based Automatic Objects Carrying and Counting System | U Bawk La Lecturer | 2020 |
1. Classical Literature 2. Modern Literature 3. Literary Theory and Criticism 4. Linguistics 5. Ancient Language 6. Indigenous Languages |
Year | Total |
---|---|
First | 112 |
Second | 85 |
Third | 41 |
Fourth | 68 |
First Year Hons: | 30 |
Second Year Hons: | 26 |
Third Year Hons: | 14 |
Qualify | 7 |
MI | 14 |
MII | 17 |
Total | 414 |
Year | Total |
---|---|
First | 20 |
Second | 24 |
Third | 21 |
Fourth | 1 |
Total | 66 |
Curriculum and Time Table
- First Year
- Second Year
- Third Year
- Fourth Year
- First Year(Hons:)
- Second Year(Hons:)
- Third Year(Hons:)
- Qualifying
- MSc First Year
- MSc Second Year
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | မ-၁၀၀၁ | မြန်မာစာ | 3 | 2 | 2 | |
2. | Eng 1001 | English | 3 | 2 | 2 | |
3. | Phys 1101 | General Physics I | 4 | 3 | 2 | |
4. | Elective (1) | * | 3 | 2 | 2 | |
5. | Elective (2) | * | 3 | 2 | 2 | |
6. | Elective (3) | Aspects of Myanmar | 3 | 2 | 2 | |
Total | 19 | 13 | 12 |
Sample Description
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | မ-၁၀၀၂ | မြန်မာစာ | 3 | 2 | 2 | |
2. | Eng 1002 | English | 3 | 2 | 2 | |
3. | Phys 1102 | General Physics II | 4 | 3 | 2 | |
4. | Elective (1) | * | 3 | 2 | 2 | |
5. | Elective (2) | * | 3 | 2 | 2 | |
6. | Elective (3) | Aspects of Myanmar | 3 | 2 | 2 | |
Total | 19 | 13 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Eng 2001 | English | 3 | 2 | 2 | |
2. | Phys 2101 | Mathematical Physics | 4 | 3 | 2 | |
3. | Phys 2103 | Electric and Magnetic Fields | 4 | 3 | 2 | |
4. | Phys 2105 | Atomic Physics | 4 | 3 | 2 | |
5. | Elective (1) | * | 3 | 2 | 2 | |
6. | Elective (2) | * | 3 | 2 | 2 | |
Total | 21 | 15 | 12 |
Sample Description
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Eng 2002 | English | 3 | 2 | 2 | |
2. | Phys 2102 | Computational Physics | 4 | 3 | 2 | |
3. | Phys 2104 | Thermal Physics | 4 | 3 | 2 | |
4. | Phys 2106 | Analytical Mechanics | 4 | 3 | 2 | |
5. | Elective (1) | * | 3 | 2 | 2 | |
6. | Elective (2) | * | 3 | 2 | 2 | |
Total | 21 | 15 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Eng 3001 | English | 3 | 2 | 2 | |
2. | Phys 3101 | AC Circuits & Electronics | 4 | 3 | 2 | |
3. | Phys 3103 | Nuclear Physics | 4 | 3 | 2 | |
4. | Phys 3105 | Classical Mechanics | 4 | 3 | 2 | |
5. | Phys 3107 | Electromagnetic Wave Theory | 4 | 3 | 2 | |
6. | Elective | * | 3 | 2 | 2 | |
Total | 22 | 16 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Eng 3002 | English | 3 | 2 | 2 | |
2. | Phys 3102 | Electronics | 4 | 3 | 2 | |
3. | Phys 3104 | Nuclear Physics | 4 | 3 | 2 | |
4. | Phys 3106 | Classical Mechanics | 4 | 3 | 2 | |
5. | Phys 3108 | Electromagnetic Wave Theory | 4 | 3 | 2 | |
6. | Elective | * | 3 | 2 | 2 | |
Total | 22 | 16 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Eng 4001 | English | 3 | 2 | 2 | |
2. | Phys 4101 | Electronics | 4 | 3 | 2 | |
3. | Phys 4103 | Nuclear Physics | 4 | 3 | 2 | |
4. | Phys 4105 | Quantum Mechanics | 4 | 3 | 2 | |
5. | Phys 4107 | Condensed Matter Physics | 4 | 3 | 2 | |
6. | Phys 4109 | Theoretical Physics | 4 | 3 | 2 | |
Total | 23 | 17 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Eng 4002 | English | 3 | 2 | 2 | |
2. | Phys 4102 | Electronics | 4 | 3 | 2 | |
3. | Phys 4104 | Nuclear Physics | 4 | 3 | 2 | |
4. | Phys 4106 | Quantum Mechanics | 4 | 3 | 2 | |
5. | Phys 4108 | Condensed Matter Physics | 4 | 3 | 2 | |
6. | Phys 4110 | Theoretical Physics | 4 | 3 | 2 | |
Total | 23 | 17 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Eng 3001 | English | 3 | 2 | 2 | |
2. | Phys 3201 | AC Circuits & Electronics | 4 | 3 | 2 | |
3. | Phys 3203 | Nuclear Physics | 4 | 3 | 2 | |
4. | Phys 3205 | Classical Mechanics | 4 | 3 | 2 | |
5. | Phys 3207 | Electromagnetic Wave Theory | 4 | 3 | 2 | |
6. | Elective | * | 3 | 2 | 2 | |
Total | 22 | 16 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Eng 3002 | English | 3 | 2 | 2 | |
2. | Phys 3202 | Electronics | 4 | 3 | 2 | |
3. | Phys 3204 | Nuclear Physics | 4 | 3 | 2 | |
4. | Phys 3206 | Classical Mechanics | 4 | 3 | 2 | |
5. | Phys 3208 | Electromagnetic Wave Theory | 4 | 3 | 2 | |
6. | Elective | * | 3 | 2 | 2 | |
Total | 22 | 16 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Eng 4001 | English | 3 | 2 | 2 | |
2. | Phys 4201 | Electronics | 4 | 3 | 2 | |
3. | Phys 4203 | Nuclear Physics | 4 | 3 | 2 | |
4. | Phys 4205 | Quantum Mechanics | 4 | 3 | 2 | |
5. | Phys 4207 | Condensed Matter Physics | 4 | 3 | 2 | |
6. | Phys 4209 | Theoretical Physics | 4 | 3 | 2 | |
Total | 23 | 17 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Eng 4002 | English | 3 | 2 | 2 | |
2. | Phys 4202 | Electronics | 4 | 3 | 2 | |
3. | Phys 4204 | Nuclear Physics | 4 | 3 | 2 | |
4. | Phys 4206 | Quantum Mechanics | 4 | 3 | 2 | |
5. | Phys 4208 | Condensed Matter Physics | 4 | 3 | 2 | |
6. | Phys 4210 | Theoretical Physics | 4 | 3 | 2 | |
Total | 23 | 17 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Phys 5201 | Electronics | 4 | 3 | 2 | |
2. | Phys 5203 | Nuclear Physics | 4 | 3 | 2 | |
3. | Phys 5205 | Quantum Mechanics | 4 | 3 | 2 | |
4. | Phys 5207 | Condensed Matter Physics | 4 | 3 | 2 | |
5. | Phys 5209 | Electromagnetic Wave Theory | 4 | 3 | 2 | |
6. | Phys 5211 | Mathematical Physics | 4 | 3 | 2 | |
Total | 24 | 18 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Phys 5202 | Electronics | 4 | 3 | 2 | |
2. | Phys 5204 | Nuclear Physics | 4 | 3 | 2 | |
3. | Phys 5206 | Quantum Mechanics | 4 | 3 | 2 | |
4. | Phys 5208 | Condensed Matter Physics | 4 | 3 | 2 | |
5. | Phys 5210 | Electromagnetic Wave Theory | 4 | 3 | 2 | |
6. | Phys 5212 | Mathematical Physics | 4 | 3 | 2 | |
Total | 24 | 18 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Phys 5201 | Electronics | 4 | 3 | 2 | |
2. | Phys 5203 | Nuclear Physics | 4 | 3 | 2 | |
3. | Phys 5205 | Quantum Mechanics | 4 | 3 | 2 | |
4. | Phys 5207 | Condensed Matter Physics | 4 | 3 | 2 | |
5. | Phys 5209 | Electromagnetic Wave Theory | 4 | 3 | 2 | |
6. | Phys 5211 | Mathematical Physics | 4 | 3 | 2 | |
Total | 24 | 18 | 12 |
Sample Description
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Phys 5201 | Electronics | 4 | 3 | 2 | |
2. | Phys 5203 | Nuclear Physics | 4 | 3 | 2 | |
3. | Phys 5205 | Quantum Mechanics | 4 | 3 | 2 | |
4. | Phys 5207 | Condensed Matter Physics | 4 | 3 | 2 | |
5. | Phys 5209 | Electromagnetic Wave Theory | 4 | 3 | 2 | |
6. | Phys 5211 | Mathematical Physics | 4 | 3 | 2 | |
Total | 24 | 18 | 12 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Ph 611 | Quantum Mechanics | 4 | 4 | 2 | |
2. | Ph 612 | Condensed Matter Physics | 4 | 4 | 2 | |
3. | Ph 613 | Nuclear Physics | 4 | 4 | 2 | |
4. | Ph 614 | Electronics | 4 | 4 | 2 | |
Total | 16 | 16 | 8 |
No. | Module No | Name of Module | Credit Points | Hours per week | ||
---|---|---|---|---|---|---|
Lecture | Tutorial | |||||
1. | Ph 621 | Quantum Mechanics | 4 | 4 | 2 | |
2. | Ph 622 | Condensed Matter Physics | 4 | 4 | 2 | |
3. | Ph 623 | Nuclear Physics | 4 | 4 | 2 | |
4. | Ph 624 | Electronics | 4 | 4 | 2 | |
Total | 16 | 16 | 8 |
No. | Module No | Name of Module | Credit Points | |
---|---|---|---|---|
1. | Ph 635 | Research & Seminar 1 | 4 | |
2. | Ph 636 | Research & Seminar 2 | 4 | |
3. | Ph 637 | Research & Progress Report | 4 | |
4. | Ph 638 | Research Outline &Their Presentation | 4 | |
Total | 16 |
Sample Description
No. | Module No | Name of Module | Credit Points | |
---|---|---|---|---|
1. | Ph 641 | Research & Seminar | 8 | |
2. | Ph 642 | Thesis & Viva Voce | 8 | |
Total | 16 |