<?xml version="1.0" encoding="UTF-8"?>
<feed xmlns="http://www.w3.org/2005/Atom" xmlns:dc="http://purl.org/dc/elements/1.1/">
<title>Department of Physics</title>
<link href="http://41.89.164.27:8080/xmlui/handle/123456789/211" rel="alternate"/>
<subtitle/>
<id>http://41.89.164.27:8080/xmlui/handle/123456789/211</id>
<updated>2026-06-15T02:25:32Z</updated>
<dc:date>2026-06-15T02:25:32Z</dc:date>
<entry>
<title>THE POTENTIAL OF KENYA'S SUSTAINABLE ENERGY TO EXCLUSIVELY MEET ELECTRIC VEHICLES ELECTRICITY  DEMAND</title>
<link href="http://41.89.164.27:8080/xmlui/handle/123456789/2770" rel="alternate"/>
<author>
<name>KIPSANG, ROGERS</name>
</author>
<id>http://41.89.164.27:8080/xmlui/handle/123456789/2770</id>
<updated>2026-06-11T08:47:44Z</updated>
<published>2025-01-01T00:00:00Z</published>
<summary type="text">THE POTENTIAL OF KENYA'S SUSTAINABLE ENERGY TO EXCLUSIVELY MEET ELECTRIC VEHICLES ELECTRICITY  DEMAND
KIPSANG, ROGERS
This study investigates the potential of sustainable energy resources to exclusively satisfy&#13;
the electrical energy demand of electric vehicles (EVs) in Kenya by examining vehicle&#13;
growth dynamics, charging infrastructure development, and projected electricity&#13;
requirements up to 2063 in tandem with Africa’s AGENDA 2063 initiative. Analysis of&#13;
fleet data shows that internal combustion engine vehicles (ICEVs) remain dominant,&#13;
expanding from approximately 1.4 million units in 2010 to 4.88 million in 2024, while&#13;
EVs adoption, which began in 2016, reached 9,019 units by 2024, with motorcycles&#13;
accounting for nearly 90% of registrations. Although EVs currently represent only 0.02%&#13;
of the national fleet, their accelerated growth since 2021 is supported by rising fuel&#13;
prices, supportive policies, heightened environmental awareness, and gradual&#13;
improvements in charging infrastructure. Projections from the regression analysis of&#13;
historical data up to 2024 suggest that the number of EVs could reach 8.2 million by&#13;
2063. On the other hand, projection using Logistic Growth Model (LGM), which&#13;
theoretically describes diffusion of an innovation in the society, predicts that the number&#13;
of EVs by 2063 could reach 5087062, 9246810, 10795415 and 11122187 respectively for&#13;
conservative (25%), moderate (50%), optimistic (75%) and original (100%) growth&#13;
scenarios. Thus, the EVs adaption in the country can best be described by the moderate&#13;
scenario because it closely matches that from regression analysis of historical data with a&#13;
deviation of 12.8%. The evaluation of charging infrastructure reveals that facilities&#13;
remain highly uneven and urban-centric, with Nairobi dominating while peripheral&#13;
regions lag behind; BasiGo, Holy Family Basilica, and Charge Net lead the sector, and&#13;
Level 2 charging is most common, with limited Level 3 and no Level 1 installations,&#13;
suggesting a strategic prioritization of mid-tier charging technologies but highlighting the&#13;
need for regionally inclusive infrastructure. Projected electricity demand from EVs varies&#13;
between 24.33 TWh and 53.19 TWh by 2063, and when combined with domestic and&#13;
industrial growth, national requirements could reach between 54.25 TWh and 83.11&#13;
TWh, equivalent to 6193 – 9488 MW. Kenya’s renewable energy capacity is projected to&#13;
grow from 2323 MW in 2024 to 6887 MW by 2063, hence will be insufficient to meet&#13;
the highest projected demand with a deficit of 2601 MW. Fortunately, the country&#13;
possesses vast untapped sustainable energy reserves that are technically viable such as&#13;
micro-hydro, geothermal, wind and solar energy. Therefore, with timely investment,&#13;
policy intervention, and nationally balanced infrastructure planning, Kenya has the&#13;
potential to meet future EVs’ electricity demand entirely through sustainable energy&#13;
resources, thereby supporting a transition towards a clean and low-carbon transport&#13;
system.
</summary>
<dc:date>2025-01-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>The Comparison between Inquiry-Based and Traditional Learning  Approaches on the Student Performance in Physics in Kesses Sub- County, Kenya</title>
<link href="http://41.89.164.27:8080/xmlui/handle/123456789/2494" rel="alternate"/>
<author>
<name>Kimiru, Kinyanjui Godfrey</name>
</author>
<author>
<name>. Samikwo, Dinah C.</name>
</author>
<author>
<name>Choge, Dismas</name>
</author>
<id>http://41.89.164.27:8080/xmlui/handle/123456789/2494</id>
<updated>2026-03-05T12:53:52Z</updated>
<published>2025-09-01T00:00:00Z</published>
<summary type="text">The Comparison between Inquiry-Based and Traditional Learning  Approaches on the Student Performance in Physics in Kesses Sub- County, Kenya
Kimiru, Kinyanjui Godfrey; . Samikwo, Dinah C.; Choge, Dismas
Physics is one of the science subjects offered in the Kenyan secondary school curriculum. Despite attracting few learners over a long period of time, its performance&#13;
has been poor as indicated in the Kenya National Examinations Council (KNEC) reports. This study aimed at investigating performance comparison between&#13;
learners taught using the Inquiry-Based Learning (IBL) approach and those taught using Traditional Learning (TL) approaches in Secondary schools within Kesses&#13;
Sub- County in Uasin Gishu County. The objective of the study was to compare the performance of students taught Physics using the IBL approach and those taught&#13;
using TL approaches. The study was based on Experiential Learning theory by Carl Rogers (1969). The IBL approach for this study was an exploratory learning&#13;
approach, which involves learners performing experiments and sharing results. The target population was 1,009 Form Three Physics students from 47 schools.&#13;
Stratified random sampling, simple random sampling and purposive sampling were used in this study. Stratified random sampling was used to divide schools into&#13;
three strata according to their categories. From each stratum, random sampling was used to select schools from the categories; extra county, County and Subcounty&#13;
schools. The sample size comprised of 282 physics students from sampled schools. A quasi-experimental design was employed where sampled students were&#13;
divided into control and experimental groups. Pre-tests and post tests were then administered and tests results were analyzed. Collected data was analyzed using&#13;
softwares which were, SPSS version 25 and the Microsoft Excel 2021 version application programs. The findings showed that performance of learners taught&#13;
Physics using IBL approach was greater than that of those taught using traditional approaches. The results of the study are expected to be instrumental to curriculum&#13;
developers at the Kenya Institute of Curriculum Development (KICD) in designing a Physics curriculum that promotes the IBL approach in delivering instructions.&#13;
The results will also help school administrators and teachers of Physics in coming up with policies that promote use of IBL approach.
</summary>
<dc:date>2025-09-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>Wavelength reuse in passive optical network for polarization based environmental sensing</title>
<link href="http://41.89.164.27:8080/xmlui/handle/123456789/2410" rel="alternate"/>
<author>
<name>Cherutoi, Henry C.</name>
</author>
<author>
<name>et. al...</name>
</author>
<id>http://41.89.164.27:8080/xmlui/handle/123456789/2410</id>
<updated>2025-06-04T07:51:45Z</updated>
<published>2024-01-01T00:00:00Z</published>
<summary type="text">Wavelength reuse in passive optical network for polarization based environmental sensing
Cherutoi, Henry C.; et. al...
We propose and experimentally demonstrate a&#13;
cost-effective technique of optical sensor that utilizes the reused&#13;
wavelength in the customer’s premises. This has been achieved by&#13;
utilizing the saturated EDFA to suppress the extinction ratio of the&#13;
incoming optical signal hence erasing the downstream data&#13;
allowing for channel reuse. A 1550nm distributed feedback (DFB)&#13;
laser is directly modulated with a 10 Gbit/s NRZ data signal and&#13;
used to characterize the erasing functionality of EDFA. The&#13;
performance evaluation is done for different input power into the&#13;
EDFA. The EDFA is shown to reduce the extinction ratio of the&#13;
incoming signal from 6.48 dB to 0.81dB when the input powers of&#13;
-7.3 dBm and 1.1 dBm were respectively used, therefore&#13;
facilitating the direct reuse of the downstream carrier. The&#13;
vibrational sensor was demonstrated at 85 MHz and the signal was&#13;
fully recovered. These results indicated the ability of the sensor to&#13;
detect a change in the environment, therefore giving an early&#13;
warning signal. The optical fiber sensor system proved to be a&#13;
reliable and cheaper alternative for environmental monitoring&#13;
utilizing re-used wavelength.
</summary>
<dc:date>2024-01-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>Parameters of Magic-Angle Twisted Bilayer  Graphene (MATBG) Superconductors</title>
<link href="http://41.89.164.27:8080/xmlui/handle/123456789/2323" rel="alternate"/>
<author>
<name>Kiboi, Dismas Chenge</name>
</author>
<author>
<name>Kapil, Mohan Khanna</name>
</author>
<id>http://41.89.164.27:8080/xmlui/handle/123456789/2323</id>
<updated>2025-05-12T08:34:12Z</updated>
<published>2023-01-01T00:00:00Z</published>
<summary type="text">Parameters of Magic-Angle Twisted Bilayer  Graphene (MATBG) Superconductors
Kiboi, Dismas Chenge; Kapil, Mohan Khanna
In general, a superconducting state is described by three critical parameters, such as, critical &#13;
transition temperature (Tc), critical magnetic field (Hc), and critical current density (Jc) or density of &#13;
states at the Fermi surface of the superconductor. In the case of Magic-angle-twisted-bilayer-graphene &#13;
(MATBG), the angle of twist ( )&#13;
 &#13;
 kT&#13;
 =&#13;
 Constant&#13;
 between the two layers of graphene is another important parameter &#13;
since the variation in  changes the value of Tc, and by virtue of the relation between Tc and EF (Fermi &#13;
energy), &#13;
&#13;
 of states ( )&#13;
 D&#13;
 E&#13;
 F&#13;
 E&#13;
 F&#13;
 the value of F&#13;
 E&#13;
 changes. Change in F&#13;
 E&#13;
 can result in the change in density &#13;
, and thus it can affect the current density. Hence in MATBG, the magic angle( )&#13;
 &#13;
 of &#13;
twist between the graphene layers becomes an essential parameter along with the three parameters ( c&#13;
 T&#13;
 H&#13;
 c&#13;
 , and c&#13;
 J&#13;
 , &#13;
) that influence superconductivity in such materials, and the parameters are calculated for &#13;
MATBG.
</summary>
<dc:date>2023-01-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>ELECTRON-HOLE SUPERCONDUCTIVITY   IN BI-LAYER GRAPHENE SUPERCONDUCTORS</title>
<link href="http://41.89.164.27:8080/xmlui/handle/123456789/2322" rel="alternate"/>
<author>
<name>Chenge, Kiboi D.</name>
</author>
<author>
<name>et. al...</name>
</author>
<id>http://41.89.164.27:8080/xmlui/handle/123456789/2322</id>
<updated>2025-05-12T08:28:57Z</updated>
<published>2023-01-01T00:00:00Z</published>
<summary type="text">ELECTRON-HOLE SUPERCONDUCTIVITY   IN BI-LAYER GRAPHENE SUPERCONDUCTORS
Chenge, Kiboi D.; et. al...
Superconductivity has been discovered in many different types of materials, such as metals, &#13;
metallic alloys, doped semiconductors, cuprate oxides, heavy fermion superconductors, and so &#13;
on; and now recently bi-layer and trilayer graphene superconductors. What is common among &#13;
all these superconductors is that the super-current is due to the frictionless flow of pairs of &#13;
charge carriers, called Cooper pairs, and the charge carriers can be electrons, holes in pairs, or &#13;
electron-hole pairs. In this manuscript, the role of electron-hole pairs in determining the &#13;
superconductivity in bi-layer graphene superconductors is studied theoretically. It is based on &#13;
the spontaneous inter-layer phase coherence in a bi-layer quantum Hall system studied using &#13;
graphene layers. The phase coherence state is assumed to be a gas of super-fluid electron-hole &#13;
pairs whose components (electrons and holes) belong to two different layers which are one &#13;
above the other and are separated by a dielectric of a very small thickness (d), and the value of &#13;
d, should be such that the state of phase coherence is not disturbed.  For such a superconductor, &#13;
specific heat (Cv), entropy (S), and transition temperature (Tc) have been calculated and &#13;
compared with values known so far
</summary>
<dc:date>2023-01-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>ANFIS-Controlled Boost and Bidirectional Buck-Boost DC-DC Converters for Solar PV, Fuel Cell, and BESS-Based Microgrid Application</title>
<link href="http://41.89.164.27:8080/xmlui/handle/123456789/2175" rel="alternate"/>
<author>
<name>Aeggegn, Dessalegn Bitew</name>
</author>
<author>
<name>et. al...</name>
</author>
<id>http://41.89.164.27:8080/xmlui/handle/123456789/2175</id>
<updated>2025-02-03T07:26:45Z</updated>
<published>2024-07-01T00:00:00Z</published>
<summary type="text">ANFIS-Controlled Boost and Bidirectional Buck-Boost DC-DC Converters for Solar PV, Fuel Cell, and BESS-Based Microgrid Application
Aeggegn, Dessalegn Bitew; et. al...
DC-DC converters are essential for integrating distributed energy resources into microgrid (MG) systems. Tese converters are&#13;
designed to incorporate intermittent renewable energy sources such as solar photovoltaic (PV) panels, fuel cells (FCs), and battery&#13;
energy storage systems (BESSs) into the grid. However, conventional DC-DC converters have limitations including lower ef-&#13;
fciency, voltage ripple, insufcient voltage regulation, and compatibility issues. Tis article presents boost and bidirectional buck-&#13;
boost converters for direct current microgrid (DCMG) applications, employing an adaptive neuro-fuzzy inference system&#13;
(ANFIS) for control. Tese proposed converter confgurations adeptly manage wide input voltage fuctuations from intermittent&#13;
sources, consistently supplying power to the DC bus at 500 V and 120 V for boost and buck operations, respectively, with an&#13;
efciency of 98.8%. Te output voltage result shows that the ANFIS-based boost converter has 10% overshoot as compared to 41%&#13;
and 50% overshoot in proportional integral (PI) and fuzzy logic controller (FLC), respectively. In both buck and boost modes, the&#13;
converters’ voltage gain is infuenced by duty ratio adjustments only, not sensitive to dynamic input voltage and fexible&#13;
manipulation of the output voltage for BESS charging. Moreover, the designed converters accommodate load variations within the&#13;
MG. To assess the converters’ ability to regulate output voltage efectively, PI, FLC, and ANFIS controllers are implemented and&#13;
compared. And the ANFIS controller demonstrates superior performance, ofering faster response times and enhanced stability.&#13;
Evaluations are conducted through simulations in the MATLAB/Simulink environment.
</summary>
<dc:date>2024-07-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>Coherent High-Speed Signal Transmission in Passive Optical Networks</title>
<link href="http://41.89.164.27:8080/xmlui/handle/123456789/2100" rel="alternate"/>
<author>
<name>Cherutoi, Henry</name>
</author>
<author>
<name>Waswa, David</name>
</author>
<author>
<name>Choge, Dismas</name>
</author>
<id>http://41.89.164.27:8080/xmlui/handle/123456789/2100</id>
<updated>2024-02-09T09:46:38Z</updated>
<published>2023-11-01T00:00:00Z</published>
<summary type="text">Coherent High-Speed Signal Transmission in Passive Optical Networks
Cherutoi, Henry; Waswa, David; Choge, Dismas
A comparative study of digital M-ary Quadrature Amplitude Modulation (16-QAM) and QPSK  modulationformats  for  high-speed  transmission  is  presented.  Based  on  VPI optical  simulation  software.  This  paper  builds  a  high-bit  rate  dual  polarization  (DP) QPSK  and16-QAM  modulation  formats  coherent  optical  transmission  system  for Passive  Optical  Networks  (PON).  Higher-order  modulation  formats  could  be  used  to provide huge data capacity, extended coverage, and long-reach connections. Channel impairments  are  mitigated  by  using  digital  signal  processing  (DSP)  for  dispersion compensation,   carrier   frequency   recovery,   and   carrier   phase   estimation.   The performance of our system is analysed on Bit Error Rate (BER=1e-9), the threshold for a communication system. For a 32-Splitter PON configuration operating with 16-QAM modulation  format,  a  data  rate  of  80  Gb/s  per  ONU is  achieved  after  24km  using standard single mode fibre (SSMF). The results indicate that the proposed schemes are a promising solution for coherent high-speed transmission in PONs.
</summary>
<dc:date>2023-11-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>Mechanical and Elastic Properties of Selected 211 MAX Phases: A Density Functional Theory Study</title>
<link href="http://41.89.164.27:8080/xmlui/handle/123456789/2086" rel="alternate"/>
<author>
<name>ARUSEI, Geoffrey</name>
</author>
<author>
<name>et al.</name>
</author>
<id>http://41.89.164.27:8080/xmlui/handle/123456789/2086</id>
<updated>2024-02-08T07:07:46Z</updated>
<published>2023-10-01T00:00:00Z</published>
<summary type="text">Mechanical and Elastic Properties of Selected 211 MAX Phases: A Density Functional Theory Study
ARUSEI, Geoffrey; et al.
MAX Phases are a class of ternary materials that have continued to play a greater role in the field&#13;
of materials science due to their unique properties that bridge the gap between metals and ceramics&#13;
which have uses in a wide range of applications. However, in spite of these progress, there are still&#13;
a lot of open questions and properties that needs to be understood. The Mechanical and elastic&#13;
properties of (Nine) MAX phase materials, namely, Ti2AlC, Ti2AlN, Ti2GaC, Ti2GaN, Ti2PbC,&#13;
Ti2CdC, Ti2SiC, Ti2GeC and Ti2SnC have been investigated using the density functional theory&#13;
within the generalized gradient approximations as expressed in Quantum Espresso and VASP&#13;
codes. The values of elastic anisotropy, Young’s modulus, Poisson ratio and shear modulus&#13;
revealed that the compounds were indeed stable and ductile. Out of all the nine MAX Phase&#13;
materials, Ti2PbC and Ti2CdC are more stable than the other considered compounds. The findings&#13;
of this study suggest that the nine MAX phases are potential candidates in various industrial&#13;
applications requiring hard materials.
</summary>
<dc:date>2023-10-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>IN SITU TECHNO-ENVIROECONOMIC ANALYSIS OF A ROOFTOP PHOTOVOLTAIC (PV) BACKUP SYSTEM IN THE TROPICAL CLIMATE</title>
<link href="http://41.89.164.27:8080/xmlui/handle/123456789/1743" rel="alternate"/>
<author>
<name>CHERUIYOT, WILKINS KOSGEI</name>
</author>
<id>http://41.89.164.27:8080/xmlui/handle/123456789/1743</id>
<updated>2023-02-15T09:33:12Z</updated>
<published>2022-07-01T00:00:00Z</published>
<summary type="text">IN SITU TECHNO-ENVIROECONOMIC ANALYSIS OF A ROOFTOP PHOTOVOLTAIC (PV) BACKUP SYSTEM IN THE TROPICAL CLIMATE
CHERUIYOT, WILKINS KOSGEI
Solar PV generators are increasingly being deployed in the built environment as stand-alone or backup power systems to supply electricity either solely or during power outages respectively. Diesel generators (DGs) are applied routinely as standby power systems by many enterprises and institutions, especially in developing countries where power outages are real and frequent due to unstable national grids. The current pursuit of low-carbon and sustainable source of energy places photovoltaic (PV) power system in advantageous position as a substitute for a DG backup system. An existing off-grid 780 Wp PV system installed as a backup power supply in a learning institution in western part of Kenya was studied both experimentally and theoretically. Technical, economic and environmental analyses were carried out to determine its performance under the local outdoor conditions at the site for a period of one year in 2020. Irradiance estimation models were also validated by experimental data to determine appropriate model(s) for the site. Plane-of-array (POA) solar radiation was measured with solar cell sensor installed at the surface of PV modules and a charge controller/inverter unit with the capability to measure and log real time output current (I) and voltage (V) was used to generate I-V characteristic data. PVsyst software was used to simulate the PV system and generate optimized theoretical results for the site which were compared with experimental results. Available energy was determined as 3202.80 kWh/year, average array efficiency of 11.71%, FF of 0.66, array yield of 4.89 kWh/kW, reference yield of 5.51 kWh/kW, capacity factor as 19.8%, annual average performance ratio (PR) as 76.0%, and average array losses as 0.54 kWh/kW. Economic results for the PV system show that the payback time (PBT) is∼ 6.38 years, LCC of $3057.93, levelized cost of energy (LCOE) of0.045 $/kWh and operation and maintenance (O&amp;M) is17.32 $/year. For the diesel generator (DG),PBT was 4.25 years and O&amp;M was 262.80 $/year for a lifespan of 5 years and assuming that it operates 2 hours per day of blackouts, LCC of $7792.75 and LCOE of 0.324 $/kWh. Environmental results show that the total annual amount of CO2 emissions avoided when PV is used instead of DG power backup system was 5.84 tCO2/year giving an average cost parameter (penalty for CO2 generation) of $9.62. Simulation results gave the available energy as 3746.40 kWh/year, reference yield of 5.55 kWh/kW, array yield of 4.18 kWh/kW, array losses of 0.61 kWh/kW, capacity factor as 21.23%, FF as 0.68, PR as 73.6% and PV array efficiency of 13.19%. The average amount of CO2 emission avoided was 7.95 tCO2/year with annual environmental cost of $116.18. Angstrom-Prescott and Iqbal models were found to be the most accurate for the site having the lowest values of mean absolute percentage error (MAPE) of 8.5% and 8.9% and root mean square error (RMSE) of 0.252 and 0.302 respectively. In conclusion, technically, the low FF (&lt;&lt;1) indicate that the system is not operating at its optimum, which can be attributed to how the PV system was installed. The LCOE results show that PV power is cheaper by a factor of seven than that of the diesel generator, and the amount of CO2 avoided is at least 0.44 tCO2/month. The PV power presents net benefits over diesel power in all performance indices evaluated, and hence can be used as a reliable and affordable replacement for DG backup systems in tandem to the global quest to transition to clean and sustainable energy sources and attainment of the SDGs 7 and 13.
</summary>
<dc:date>2022-07-01T00:00:00Z</dc:date>
</entry>
<entry>
<title>Ab initio insights into Graphene-Zirconium disulfide/diselenide heterostructure as electrode material for alkali-ion batteries</title>
<link href="http://41.89.164.27:8080/xmlui/handle/123456789/1605" rel="alternate"/>
<author>
<name>King’ori, Gladys W.</name>
</author>
<author>
<name>et. al...</name>
</author>
<id>http://41.89.164.27:8080/xmlui/handle/123456789/1605</id>
<updated>2022-03-28T07:26:20Z</updated>
<published>2021-01-01T00:00:00Z</published>
<summary type="text">Ab initio insights into Graphene-Zirconium disulfide/diselenide heterostructure as electrode material for alkali-ion batteries
King’ori, Gladys W.; et. al...
In the search for an energy storage medium with higher electronic conductivity, rate performance and moderate volume expansion, van der Waals heterostructures&#13;
are a promising alternative. Herein, the potential of graphene (Gr) and Zirconium dichalcogenide (ZrX2, X = S, Se) van der Waals heterostructures for applications as&#13;
battery electrodes is explored using density functional theory (DFT) calculations. Through intercalating alkali ions (Li and K) between the Gr and ZrX2, we obtain low&#13;
energy activation barriers, indicating that Gr-ZrX2 van der Waals heterostructures can be candidates for high rate performance electrode application.&#13;
DFT calculations also indicate that the Gr-ZrX2 heterostructure formation is energetically favoured with better volume expansion as compared to bilayer Gr and&#13;
ZrX2. The calculated open circuit voltage (OCV) for K intercalation was 0.66 V (Gr-ZrSe2) and 0.77 V (Gr-ZrS2), hence suitable for anodic application in Potassium-ion&#13;
batteries (KIB). The calculated OCV for Li interaction was 2.83 V (Gr-ZrSe2) and 2.95 V (Gr-ZrS2) hence suitable for cathodic applications
</summary>
<dc:date>2021-01-01T00:00:00Z</dc:date>
</entry>
</feed>
