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Classical Analogue of the Ionic Hubbard Model
In our earlier work [M. Hafez, et al., Phys. Lett. A 373 (2009) 4479] we employed the flow equation method to obtain a classical effective model from a quantum mechanical parent Hamiltonian called, the ionic Hubbard model (IHM). The classical ionic Hubbard model (CIHM) obtained in this way contains solely Fermionic occupation numbers of two species corresponding to particles with and spin, respectively. In this paper, we employ the transfer matrix method to analytically solve the CIHM at finite temperature in one dimension. In the limit of zero temperature, we find two insulating phases at large and small Coulomb interaction strength, , mediated with a gap-less metallic phase, resulting in two continuous metal-insulator transitions. Our results are further supported with Monte Carlo simulations.
pacs:71.30.+h, 68.35.Rh
I Introduction
To understand the magnetism and magnetic phenomena, one of the basic interactions is the exchange mechanism which is deeply rooted in Coulomb interactions and quantum mechanical indistinguishability. Therefore a fair understanding of the magnetic behavior of materials is not possible without investigating appropriate quantum spin models. Introducing uni-axial anisotropy to the Heisenberg model amounts to suppression of transverse quantum fluctuations (), leading to the so called Ising model Newell (). The resulting Ising Hamiltonian turns out to contain the basic magnetic phases of the original Heisenberg model, namely ferromagnetism, and antiferromagnetism Feynman (). Although many of the interesting possible aspects such as spin liquid phases, spin-wave excitations, etc. Fradkin () can not be captured by the Ising model. Classical Ising model has the merit of being much simpler to solve, and admits analytical Newell (); Onsager () and graphical solutions Feynman () in various geometries JafariIJMP () in one and two dimensions which is lacking in the original quantum Heisenberg model.
Dielectric properties are among the most important properties characterizing materials. The question can be asked here, is there any Ising-like model that can provide basic informations about their phase diagram, and at the same time being simple enough to allow for analytical solutions? We have taken the example of the (IHM) Nagaosa (); Egami (). This model was introduced to study the neutral-to-ionic transition in organic compounds, as well as, understanding the role of strong electronic correlations in the dielectric properties of metal oxides Egami (); HafezCUT (). This model is as follows:
where () is the usual annihilation (creation) operator at site with spin . is the on-site Coulomb interaction parameter, and denotes a one-body staggered ionic potential. The kinetic energy scale is given by the real hopping amplitude which prefers to gain kinetic energy by spreading the wave-function over the whole system, leading to quantum fluctuation of the charge density. The zero temperature phase diagram of this model contains Mott and band insulating states when the energy scales corresponding to or dominate, respectively HafezCUT (). When these two scales become of the same order of magnitude, the nature of intermediate phase still remains controversial. Some authors argue that the intermediate state is a spontaneously broken symmetry phase SBSP (), while some others argue that the phase in between is metallic Nagaosa (); Bouadim2007 (); HafezCUT (); Metals (). In our previous investigation HafezCUT () we employed the method of flow equations for the quantum Hamiltonian (1) to obtain an effective Hamiltonian in which the hopping term is renormalized to zero, producing a new nearest neighbor Coulomb attraction. The resulting classical Hamiltonian is of the following lattice gas form:
where the renormalized parameters have closed form expressions in terms of the bare parameters HafezCUT (). We take the kinetic energy scale as the unit of energy.
By calculating the spin and charge gaps, we showed that this simple classical model is capable of capturing the physics of a metallic state sandwiched between two distinct insulating phases at zero temperature as one increases for a fixed value of HafezCUT (). Here contains two species (or colors) corresponding to , respectively. Since for each "color" is either or , it is an Ising-like variable. Therefore our effective CIHM Hamiltonian can be thought of, as two inter-penetrating Ising models on a lattice. Being a natural extension of two species lattice gas model, allows for analytical solution in one spatial dimensions (1D). Here we can employ the transfer matrix method, constructed in terms of matrices to calculate the thermodynamic properties of this model at finite temperatures. At high temperatures where the thermal fluctuations wash out the quantum effects, we expect the results of our calculations to be a good description of the class of materials modeled in terms of IHM. Also a novel graphical solution in 2D similar to Feynman's construction can be worked out JafariUnpublished ().
The paper is organized as follows: In the next section we calculate the grand canonical potential for this model in one dimension and discuss the particle density and ionicity in various fillings. It is followed by a section focused on half-filling situation, and calculate the specific heat, compressibility and ionicity to assess the nature of the phases in the parameter space of . Throughout the paper we have fixed the value of HafezCUT (). The final section is devoted to summary and discussion.
Ii Grand Potential
In this section we calculate the grand canonical potential that can be derived from the grand partition function (GPF) which is defined as follows:
where is Temperature, is lattice size, and is chemical potential. The denotes all possible configurations of the occupation numbers, which must be summed over. is the number of particle and is the energy that is defined by the model Hamiltonian Eq. (2).
The summation in Eq. (3) can be calculated analytically as follows. The values of are only zero and one, which is the Fermionic memory left in the commuting variables . Hence , and the second term in Eq. (2) becomes:
The GPF becomes,
As can be seen at the Hamiltonian level, only the spin-summed occupations appear and therefore this classical model does not contain spin-polarized (magnetic) solutions. So we change the summation variable from and to that has three possible values 0,1,2. Therefore we have:
where the coefficient takes into account the two-fold degeneracy for in Eq. (5), which corresponds to either , , or , . Eq. (6) can be written in a more symmetric form,
where is assumed to be even and the periodic boundary conditions, is implied. Defining the matrix elements of the transfer matrix by,
Eq. (7) can be written as:
where is the transpose of , . Then the partition becomes:
where , , and are the eigenvalues of . In the thermodynamic limit where is very large, the grand potential per site becomes:
Here is the maximum eigenvalue. Hence to obtain the grand potential one needs to calculate the eigenvalues of . Later on, when we discuss the ionicity, we will in addition need the eigenvectors of . The eigenvalues of are solutions to the third order equation,
with , , and given in the appendix. Through the paper we will report the numerical plots for in units in which . For this value of , there would be no level-crossing among the eigenvalues of the matrix when one varies , , and , as expected from Perron's theorem Goldenfeld ().
From the partition function, one can in principle calculate various averages of the form . The simplest of these averages are the average particle density (symmetric combination), and the ionicity (antisymmetric combination) which contain important information about the nature of the thermodynamic phases of the model. In the following we calculate these averages as a function of .
ii.1 Particle Density
Once the grand potential is known, one can derive many other thermodynamic quantities. The particle density, , can be calculated as,
In Fig. 1, the particle density versus has been plotted for different values of . In this figure the value of is fixed to be . This value of corresponds to a band insulating regime at zero temperature HafezCUT (). As can be seen in the figure, apart from trivial cases of the empty () and the fully-filled () lattice, there are three plateaus. The first one corresponds to the half-filling (i.e. one particle per lattice site), and two others correspond to commensurate fillings, (quarter-filling), (three-quarter-filling) which is quite similar to the plateaus of the parent ionic Hubbard model Bouadim2007 (). Indeed the and are related by a particle-hole transformation. Therefore in what follows, we focus on . With increasing the temperature, the plateaus get more and more rounded. The value of chemical potential corresponding to the half-filling is independent of temperature, as can be seen in Fig. 1. The inset plot indicates this point more transparently. This "isosbestic" behavior is observed for all values of values of .
In Fig. 2, we have plotted the particle density as a function of chemical potential at a constant (low) temperature , for different values of . As can be seen in the figure, increasing , causes the plateaus which are particle-hole counterpart of each other, get wider. However the plateau at gets narrower and finally vanishes around , resulting in a gap-less phase at half-filling. Upon further increasing , the half-filling plateau is recovered, and gets wider, indicating the emergence of a growing new gap in the system, which is reminiscent of the Mott insulating behavior. To identify the nature of gap at one needs to calculate the ionicity, which provides information about how the unit cell is being filled. This will be done in the sequel.
For later reference, we report the value of chemical potential corresponding to half-filling, which by examining the numerical plots turns out to be:
The temperature range at which the above relation is valid, is roughly . For temperatures outside this range, there will be deviations from the above rule of thumb relation.
ii.2 Ionicity
If denote the sublattice of odd and even sites, respectively, then and are defined as:
the ionicity per site becomes , where , and is the total number of lattice sites. This quantity can also be calculated analytically with the aid of transfer matrices. In the grand canonical ensemble is given by:
Depending on whether is odd or even, similar to calculations for grand partition function, we obtain:
where is the following matrix:
In Fig. 3, we have plotted the ionicity per site as a function of for various temperatures at a fixed value of . For this value of , at zero temperature one would expect a band insulator at half-filling, where A-sublattice (with on-site energy ) are doubly occupied. Let us focus around which corresponds to quarter filling (c.f. Fig. 1). The value of for in Fig. 3 shows that the only electron of each unit cell belongs to A-sublattice, which represents a charge density wave insulator.
As we increase from , the ionicity increases, which indicates that sublattice A continues to be filled. When , one approaches the half-filling (Fig. 1), where at lower temperatures the A-sublattice is totally occupied, hence . As can be seen in Fig. 3, this saturation value is decreased as the temperature is increased. This reduction in the ionicity, indicates that the particles are bing thermally excited across the band gap. Further increasing of the chemical potential, one reaches the plateau around of Fig. 3 (c.f. Fig. 1). The decrease in the ionicity indicates that the added particles essentially start to occupy the B-sublattice. The symmetry of Fig. 3 around , is due to the apparent particle-hole symmetry of the Hamiltonian.
In Fig. 4 we plot the ionicity per site at the constant temperature and different values of indicated in the legend. Again there are three plateaus corresponding to 1/4,1/2 and 3/4-filling, respectively. This figure indicates that the center of the half-filling plateau is at . This can be understood as a Hartree like energy for the Hubbard model. Now concentrating around half-filling in this figure, for small values of , the ionicity reaches , which indicates a complete electric polarization of the unit cell, and hence we have a band insulator. For intermediate values of , the maximum value of ionicity does not reach , which shows some of the added particles start to occupy the B-sublattice. Also note that for the intermediate values of the half-filling plateau starts to disappear, i.e. the emergence of a metallic behavior. For large values of , the half-filling plateau is restored, but at zero ionicity. Therefore we have an insulator with unpolarized unit cell. Such an insulating state can be thought of as classical counterpart of the Mott insulating state.
Iii Half-filling
As we saw in Fig. 2, for the energy scales cooperate with each other, to give rise to a charge density wave insulating ground state. Rather at , these two energy scales compete against each other to destroy the insulating behavior for intermediate (), giving rise to a richer phase diagram. Therefore in this section we focus at half-filling and calculate the specific heat, compressibility, and ionicity. Before doing so, we compare some physical quantities evaluated by a fully numerical Monte Carlo simulation, with our exact transfer matrix results. In Fig. 5, ionicity and specific heat per site are plotted at half-filling and show a good agreement between analytical and numerical results. This ensures that both Monte Carlo and analytic results are reliable.
Now let us proceed with the calculation of various thermodynamic quantities. For the fixed value of , we have two ways to plot thermodynamic quantities. First way is to plot them as a function of temperature , at some selected values of . These results indicate that in the present one dimensional model, there will be no finite temperature phase transition. This is obviously due to the analytic behavior of the partition function as a function of . The second way is to plot them as a function of , for some selected temperatures. This second way of presenting the data, reveals that as one lowers the temperature, there will be sharper features as a function of , indicating the zero temperature phase transition. Our calculations are based on Eqs. (11,14). For very low temperatures, where the validity of Eq. (14), might be questioned, we employ Monte Carlo simulation data.
iii.1 Specific heat
Specific heat per site can be calculated as:
where is entropy per site at half-filling that can be derived from the grand potential. Figure 6 shows the specific heat versus for various values of . As can be seen in Fig. 6 for values of , there is a single peak in the . For a peak-dip-hump structure can be observed. For the hump is quite clear, while for , it can be interpreted as a precursor to the hump. For , the peak merges into the hump structure. In terms of the parent quantum Hamiltonian, such hump structure indicates incoherent excitations. For , Eq. (14) is not reliable at very low temperatures. Therefore we report Monte Carlo simulation results which indicates a very sharp peak at . As moves towards from both sides (lower and upper panels), the peak gets sharper and moves towards lower temperatures. This indicates that in limit one expects a transition between gaped and gap-less states.
This behavior can be simply understood in terms of a two-state model with level spacing , whose specific heat is given by
where . Behavior of Eq. (22) for is like , while for it vanishes as . For the intermediate region a Schottky peak around () arises in the specific heat. Fitting the specific data to Eq. (22), in Fig. 7 we have plotted the estimated gap versus , which indicates two gaped phases. According to the above two-state formula, this peak corresponds to , from which a gap of can be estimated. If we extrapolate the estimated gap for , zero gap region is expected to occur for which is compatible with our previous work HafezCUT ().
Now let us look at the specific heat data from a different angle. In Fig. 8 we plot the specific heat versus for different values of temperatures. As can be seen, there are two peak structures at all temperatures, which get sharper and by lowering the temperature, they tend to accumulate around . Extrapolating the trend of this double-peak structure to the limit of , suggests two phase transitions at and HafezCUT (), compatible with the behavior of the vanishing gap region in Fig. 7. The characteristic quadratic behavior around seen in Fig. 8, which according to the two-state model is expected to be like , indicates two continuous metal-insulator transitions, with , .
iii.2 Compressibility
Another quantity that can be treated in our consideration CIHM is the compressibility which is given by:
where is the density of particles per site.
In Fig. 9 we plot the compressibility as a function of for different values of . Zero compressibility is a characteristic of gaped states. As can be seen in this figure for small value of the range of temperatures at which the compressibility is close to zero is substantial, which means that the gap is so large that up to such temperature the insulating behavior is still manifest. By increasing , this temperature range shrinks and becomes smaller and smaller, until around , it extrapolates to zero. Increasing beyond , again recovers a finite temperature range in which the compressibility is zero. This behavior confirms that a gap-less state is sandwiched between two gaped states.
To see the above statement more clearly, in Fig. 10 we plot compressibility as a function of for selected temperatures.
As can be seen in this figure, there is a region with non-zero compressibility, which characterizes a gap-less phase. Outside this region, the compressibility decays to zero. By decreasing , the width of the compressibility peak becomes smaller and while the height of the peak diverges as ; a typical characteristic of a continuous phase transition. This confirms the existence of a metallic phase at zero temperature HafezCUT (). The effect of thermal fluctuations is to smear the edges of metallic region. This is quite intuitive, as for values of near the zero temperature boundary of metallic phase with neighboring insulating phases, the gaps are small, and hence the thermal energy can overcome the gap.
iii.3 Ionicity
In Fig. 11 we plot the ionicity per site for and various values of at half-filling. As can be seen in the figure, by lowering the temperature, for , the ionicity tends to ; for it reaches a zero temperature value of ; while for , it reaches a value between these two limits; characterizing a phase with charge fluctuations.
This behavior can be understood as follows: At small regime the unit cell is fully polarized at low temperatures, with both and particles occupying the A-sublattice. As the temperature is increased, some of the particles get excited to B-sublattice by absorbing the thermal energy, . Similarly for large values of , at lower temperatures the unit cell is not polarized, due to the Coulomb term . By increasing the temperature, thermal excitations with doubly occupied sites will be created, thereby increasing the ionicity. For intermediate , the weights of polarized and unpolarized configurations in the unit cell become comparable; hence giving the ionicity .
In Fig. 12 we plot the ionicity at half-filling as a function of for and various values of . As can be seen at all temperatures, the ionicity smoothly varies between for small values , and for large values of . The width of the transition region decreases by lowering the temperature, and is expected to approach the figure 2 of Ref. HafezCUT, .
Iv Conclusion
In this work we studied a classical model consisting of two Ising like variables on a one dimensional chain. Despite the simplicity which essentially results form the lack of Fermionic minus sign problem, our model captures some of the interesting properties of the ionic Hubbard model. Various thermodynamic properties, such as, specific heat, ionicity, particle density and compressibility when viewed as a function of in a given temperature, indicate the presence of two gaped states at small and large values of , with a gap-less state sandwiched between them (around ). When the same quantities viewed as a function of temperature, there is no sign of phase transition down to zero temperature. The three phase scenario of the zero temperature with clear zero temperature phase transition boundaries at and extrapolates to higher temperatures. However, the boundaries get smeared due to thermal fluctuations, giving rise to a cross-over behavior.
Mapping of dimensional quantum models to dimensional classical Hamiltonians is a well known paradigm in statistical physics. Our flow equation approach HafezCUT () suggests an alternative approach to construct "" dimensional classical models which might be useful in capturing basic aspects of the original quantum Hamiltonian.
V Acknowledgements
We would like to thank Professor N. Nafari for useful comments and critique of the manuscript. This research was supported by the Vice Chancellor for Research Affairs of the Isfahan University of Technology (IUT). S.A.J was supported by the National Elite Foundation (NEF) of Iran.
Vi Appendix
vi.1 Coefficients of Eq. (12)
The coefficients , , and of Eq. (12) are as follows:
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KUANTAN, 12 April – Director of MACC Pahang, Dep. Com. Mohamad Fauzi Husin made a courtesy call on YB Dato' Sri Haji Ishak Haji Muhamad, Yang DiPertua of Pahang State Assembly at his chambers, Wisma Sri Pahang here today.
The main focus of the discussion was the planning for a Corruption-Free Pledge ceremony with Pahang ADUN and Excos, in addition to strengthening relations and cooperation between MACC Pahang and the Pahang state government in the effort to eradicate and curb corruption, abuse of power and malpractice among politicians of Pahang state government.
Also in attendance were Deputy Director (Prevention) of MACC Pahang, AC Sheikh Hamadi Sheikh Abdul Hamid and Mr. Syed Ahmad Khirulanwar Alyahya Syed Abdul Rahman, Division Secretary of Pahang State Assembly.
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WASHINGTON, D.C. — Import cargo volume at the nation's major retail container ports is expected to see a final surge and set a new monthly record in October as the holiday season approaches, according to the monthly Global Port Tracker report released by the National Retail Federation and Hackett Associates.
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Import volume at U.S. ports covered by the Global Port Tracker report is expected to total 1.53 million containers this month, topping the 1.52 million monthly record set in August. Cargo volume has been well above average each month since spring as retailers have imported merchandise early in case of any disruption on the docks.
The contract between the Pacific Maritime Association and the International Longshore and Warehouse Union expired on July 1, prompting concerns about potential disruptions that could affect back-to-school or holiday merchandise. Dockworkers remain on the job as negotiations continue but the lack of a contract and operational issues have led to record congestion at the ports.
The 1.52 million twenty-foot equivalent units (TEUs) handled in August, the latest month for which after-the-fact numbers are available, was up 1.5 percent from July and 2.1 percent from August 2013. One TEU is one 20-foot cargo container or its equivalent.
September was estimated at 1.48 million TEU, up 2.8 percent from the same month last year, and October's forecast of 1.53 million TEU would be up 6.4 percent from last year. November is forecast at 1.39 million TEU, up 3.7 percent, and December at 1.37 million TEU, up 3.9 percent.
Those numbers would bring 2014 to a total of 17.1 million TEU, an increase of 5.3 percent over 2013's 16.2 million. Imports in 2012 totaled 15.8 million. The first half of 2014 totaled 8.3 million TEU, up 7 percent over last year.
January 2015 is forecast at 1.42 million TEU, up 3.5 percent from January 2014, while February is forecast at 1.35 million TEU, up 8.5 percent from last year.
The import numbers come as NRF is forecasting 4.1 percent holiday season sales growth and 3.6 percent growth for 2014 overall. Cargo volume does not correlate directly with sales but is a barometer of retailers' expectations.
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Bienvenido a Peru!
Flew from Lima to Cusco today! We're acclimating to the altitude for 2 days before hiking the Inca Trail. The flight in over the Andes was pretty ridic.
Off to wander! Adios!
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October 23, 2014
The Community Health Worker Network of Buffalo, along with several of our community partners, hosted a successful community forum at Canisius College withDr. Andy Coates, President of Physicians for a National Health Program headlining, exploring why the United States spends twice as much as any other country on health care, with outcomes that consistently rank 30th or worse on the World Health Organization index for health improvement.
Support for "single payer" healthcare is growing in New York State, and NYS Assembly hearings will be held across the state, including Buffalo, next month in regard to "New York Health", a universal single payer health coverage bill, which would provide comprehensive, universal health coverage for every New Yorker. Sam Magavern, Co-Director of Partnership for the Public Good, Dr. Kathleen Grimm of ECMC's Palliative Care department, and Deirdre Wright, a Community Health Worker at Jericho Road Community Health Center also provided insight into the need for a new healthcare system. Hearings on a NY "single payer" bill will be held in Buffalo onNovember 12th. Stay posted for more information!


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WHO (World Health Organization) has acknowledged that an outbreak of Coronavirus COVID-19 has turned into a true pandemic. At present there are 134 828 cases in more than 100 countries; and 4 984 people died. Meanwhile, the Director of WHO, Dr Tedros Adhanom Ghebreyesus, is quite optimistic and claims that COVID-19 still might become the first controlled pandemic in the human history.
In these conditions the International Chamber of Shipping (ICS) has issued a comprehensive guidance for seafarers and ship operators providing instructions for the crew and passengers against the disease. They recognize the danger for the maritime community exposed to the virus and inadvertently contributing to the spread due to the international nature of shipping.
The document has been prepared in cooperation with The International Maritime Health Association (IMHA), The European Centre for Disease Prevention and Control (ECDC), IMO and WHO; it contains 22 pages and is likely to become a regulation for the time of Coronavirus pandemic.
Protective Measures Onboard
It is now confirmed that Coronavirus COVID-19 is transmitted primarily by droplets released when a sick person coughs or sneezes. Therefore, crews and passengers are instructed to exercise simple hand and respiratory hygiene:
Suspected and Confirmed Cases Onboard
Meanwhile, despite the precautionary measures a crewmember or passenger might fall ill. They are considered suspect cases if:
According to ICS procedures Ship Medical Officer or Doctor should conduct an interview and if the patient falls into one of the above mentioned categories he or she should be treated as COVID-19 Suspect case.
ICS Instructions for Suspect and Confirmed Cases
1. The suspect case should be isolated into a separate cabin or ward;
2. All persons who contacted with the sick should be traced and categorized as high risk exposure (cabin mates, immediate colleagues, recently dined at the same table, etc.) and low risk exposure (have not been in close contact with a sick person). Crew members should be asked to self-monitor symptoms of COVID -19 during the next 14 days and self-isolate and report immediately should any suspicious symptoms manifest themselves.
3. Onboard cases are handled by designated medical care providers and records should include:
3.1 Interviews of suspect cases recorded in the medical log book (symptoms, travel history, concomitant diseases);
3.2 Records of anyone visiting medical facility as a high risk exposure and protective measures taken;
3.3 Contact details of low risk exposure cases if they plan to disembark (completed Passenger Locator Form (PLF) or Maritime Declarations of Health (MDHs));
3.4 Records about COVID-19 spread onboard, disinfection, etc.
4. As per the ICS procedure, the Master should alert the competent authority at the next port of call about any suspect case to ensure that facilities are available to transport, isolate, and care for the patient.
5. WHO insists that international trade should not be hampered; and cargo and crewing operations should proceed without disruptions as far as possible. However, many countries impose their own regulation and quarantine requirements. The complete map of port restrictions is here.
6. Controlled disembarkation takes place at the next port of call. The patient must wear surgical mask; while his escort should be gowned in the PPE (gloves, goggles, gown and mask).
7. The medical samples should be transferred to the laboratory for the diagnostics and their results then reported the ship officers.
8. The ship may proceed to the next port of call if competent authorities are satisfied with the following formalities:
8.1 The public health requirements at the port of call have been adhered to;
8.2 The COVID-19 suspect case has been handled in accordance with procedures and there are corresponding reports;
8.3 Contact tracing forms and PLFs (if appropriate) are filled in properly;
8.4 There has been a proper COVID-19 information campaign onboard and crewmembers are aware of symptoms and necessary precautionary actions;
8.5 Cleaning and disinfection measures in the cabin or ward have been conducted as required.
The ICS guidance is thorough as it contains not only instructions, but safety posters you can print out and pin on board; necessary PLF forms and updated list of medical supplies that should be on every vessel while the world in trying to take over the new pandemic.
Click here to Download the full text.


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Bay Area Briefs
Man killed by Caltrain
PALO ALTO – Caltrain officials report that a man was struck and killed by a northbound train this morning, and the accident will likely affect train service throughout the morning.
Caltrain spokeswoman Jayme Maltbie said the accident occurred at about 8:10 a.m. when a trespasser on the tracks was struck and killed at the Churchill Crossing in Palo Alto. The victim has not yet been identified.
Maltbie said that six trains were stopped in the Palo Alto area at 9:15 a.m. as a result of the fatality and it may take some time before service can be restored to its normal schedule as the investigation continues.
Family slain in San Jose
SAN JOSE – San Jose police said two adults and two toddlers were found shot to death in their home in east San Jose Monday afternoon.
The San Jose Police Department said a person of unknown relation discovered the family in the house at 88 Melrose Ave. and called police at 1:15 p.m. Monday.
San Jose Police Officer Joseph Deras officers were still trying to confirm the identities of the four victims, which include a 2-year-old, a 4-year-old and an adult male.
He said the victims may have been dead for over 24 hours before being discovered.
"There's an outside possibility this is a murder suicide but there could also be a suspect still outstanding,'' Deras said.
One man was detained, although it is not known why. Also, the grandmother of one of the victims was extremely upset and was removed from the scene by an ambulance Monday afternoon. Deras said a handgun was recovered near one of the bodies.
Officers had been in contact with the family over the weekend. The reason for the visits was not known.
Sat Hernandez, a neighbor, said the Portuguese family was quiet and kept to themselves.
"The street is very quiet and peaceful. I've been really comfortable here for the past 22 years. I've never had one problem with one neighbor,'' Hernandez said.
Woman sues Taco Bell, claims food poisoning
NAPA – A woman who said she was sickened by food from a Taco Bell in Napa is suing the chain seeking more than $25,000 for lost wages, medical care and compensation.
Diana Franklin is one of nearly 100 area residents who complained to the Napa County Department of Environmental Management about food poisoning from the Taco Bell. The complaints centered on food served on Mother's Day weekend at the chain's Jefferson Street location.
A department investigation placed the blame on workers who handled food with their bare hands, spreading a virus.
The lawsuit called the food handling negligent.


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Mrs. Ernestine T. Horton of 1600 Mote Road Covington, GA entered eternal rest on March 17, 2020. Services will be held Saturday, March 21, 2020, 1:00 P.M. at Early Hope Church Ministries, 1129 Rocky Plains Road Covington, GA 30016, Rev. Kenneth Williams, Pastor, Eulogist. Assisted by others. Interment Church Cemetery. She leaves to cherish her memories a host of loving family and friends. The remains will lie in-state at 11:00 A.M. until the hour of service. The family will assemble at the above address at 12:00 Noon. "A Service of Dignity, A Trademark of Excellence."
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Xtreme Monkey XM-2655 Multi Purpose Harness - Sled/Resistance
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Train like the top athletes around the world with the World Sport brand Speed and Agility Training Belt. This training device is used in the NBA, NFL, MLB, MLS, NCAA, and in almost every top soccer team around the world. Designed to develop explosive linear speed.
Includes: adjustable harness and pull cord
Item may be slightly different then what appears in the picture, as we continue to improve our products.


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Learn About Buying a Used Car
One of the greatest ways that you can save money when you are purchasing a car is by buying a used one rather than a brand new. It will become crucial for one to understand that a new car will become worthless after you have bought it since it depreciates rapidly. However, you will be able to save a couple of thousands when you let someone else absorb the depreciation by using the new car for the first new year's. Purchasing the right car with a good predictability as well as low ownership costs will also save your money over the years.
It will be important for you to understand that to get a great deal for a used car, it takes a lot of time and effort and the process is more challenging when compared to buying a new car and also, the car is not covered by nay factory warranty. Buying a pre-owned car is not one of the easiest purchase that you will make, there is a lot of uncertainty about what you are buying and thus it will take a lot of time and effort but with the right approach as well as information, then it will become much easier for you to make the right decision. Buying a car will be a great investment on your side and thus you want to ensure you get value for the price you will pay for.
You need to know that when you are buying a pre-owned car, it will be better that you buy from a dealership rather than buying from an individual since there are some benefits that come with this. It will be important for you to understand that when you are buying a used car from a dealer, you are sure that the purchase is backed up by the dealer and the vehicle will be inspected mechanically and even reconditioned and in most of these cases, these cars will come with some additional offers or warranties.
In the process of buying a used car, you ought to know that selecting the best-used car dealer to deal with happens to be the most important thing. It will be necessary that you consider finding a reliable, reputable as well as an experienced used car dealership to buy your next car from so as to make sure that you achieve the best results. There are a lot of things that one will need to check on when it comes to choosing a used car dealership.


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Qu'il nous manque, le mec 😉
This entry was posted on samedi 4 juillet 2015 at 08:42 and is filed under Amour du prochain, Souvenirs, spectacle. You can follow any responses to this entry through the RSS 2.0 feed. You can leave a response, or trackback from your own site.


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This section is a comprehensive resource for our clients, containing tax calculators, tax rates and deadlines, essential business factsheets, the latest news and more.
Includes calculators for mortgages, loans, APR, payslips, VAT, stamp duty, company car and fuel benefits.
The online tax calendar shows the key tax deadlines.
The latest tax rates and allowances.
Some useful forms from HMRC and Companies House.
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B.C. is at the "end of the beginning of this pandemic," provincial health officer Dr. Bonnie Henry said, but day to day life may not change much in the weeks ahead.
"Physical distancing has made a difference," Dr. Henry said during an epidemiology presentation today, May 4, that looked at how the pandemic has worked its way through B.C.
"It has allowed us to put the put the brakes on COVID-19, but we haven't stopped the car and it's very unlikely that we're going to be able to do that in the coming months."
So, as social interactions stay at the current 30 per of normal, and B.C. eyes opening up to 60 per cent — a number that will allow for social distancing and some resumption of normal life — Dr. Henry said that orders on the number of people allowed to gather will remain at 50, businesses will have to implement measures that make interactions safer and even outdoor visits will remain preferred.
There's so much that remains unknown about this virus and that is not just the case in B.C. or in Canada, but also around the world, she said. Until there is a vaccine social distancing will be the norm.
"The goal in the next months is to make sure that we learn how to live with this virus in a safe way that protects people this year," she said.
"We don't know yet whether we're going to have a resurgence of respiratory illness when influenza season and respiratory virus season starts again in the fall, that is something we need to plan for, we need to prepare for and we need to monitor for starting now."
In the meantime, hand hygiene, avoiding touching our faces, coughing into sleeves and disinfecting frequently touched surfaces will remain the norm.
"Those are all things that are needed, and need to stay the same — staying at home and away from others if you're feeling ill, that has to be our new normal for forever," she said.
Dr. Henry said she has faith that British Columbians will rise to the challenge.
"I think we have seen that people are very concerned about this and we have seen what's happened around the world and people know what we need to do, it's hard and it's been hard on us all collectively to get where we have," she said.
"So we all collectively have a vested interest in doing the right thing. I've said it many times, I really honestly believe that if we give people the information … we know that most people will do the right thing and I'm convinced that is the case here in B.C."
If not, the risks to medically vulnerable people in our families is high, particularly if they are male.
Men in B.C., as has been the case across the globe, are suffering more severe consequences from COVID-19, Dr. Henry said.
Dr. Henry said that across B.C., most people who've tested positive for COVID-19 have been between the ages of 30 and 60 years old, and more women have been affected.
When it comes to hospitalizations, however, there is a shift to the older age groups and men.
"Most of the people in ICU are in their 60s and 70s and, again, more men than women required that critical care," she said, adding younger people are not immune. People in their 20s and 30s have required hospitalization and been admitted to the intensive care unit.
When it comes to deaths, the majority have been people in their 70s, 80s and over 90.
"We also have seen that it's much more than half of the men over age 90 have died, whereas it's less than 20 per cent of women," she said.
"So this is a phenomenon that we're seeing around the world that men are more likely to have more severe illness to require hospitalization and to die from COVID-19, and we really don't understand why there's a lot of work going into trying to understand that phenomenon."
There have been 53 new cases of COVID-19 since Saturday bringing our total to 2,224.
Of those, 845, people are in Vancouver Coastal Health, 1,027 are in Fraser Health region, 124 people were in Vancouver Island Health, 177 in Interior Health and 51 people in the Northern Health region.
Currently, there are 77 people in B.C. who are in hospital with COVID-19 and of those 20 are currently in critical care.
There were also three more deaths over the weekend, all of them in long term care here in the province, bringing the total number of people who've died to 117.
To contact a reporter for this story, email Kathy Michaels or call 250-718-0428 or email the editor. You can also submit photos, videos or news tips to the newsroom and be entered to win a monthly prize draw.
We welcome your comments and opinions on our stories but play nice. We won't censor or delete comments unless they contain off-topic statements or links, unnecessary vulgarity, false facts, spam or obviously fake profiles. If you have any concerns about what you see in comments, email the editor in the link above.


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- Location:
Remuera, Auckland
Get directions
- Departs from:
2nd Floor, Dalmation Society Building, 10 New North Road Eden Terrace 1021 NZ
ph:00 64 9 300 7320
- Departure time:
- 8:30 am
Make a positive difference to your local stream!
Conservation Volunteers New Zealand, the ÅrÄkei and the WaitematÄ Local Boards are working together with local communities to restore the Newmarket stream. The restoration efforts include getting rid of invasive weeds and replanting the stream banks with native plants. A natural, clean and beautiful stream environment is good for native wildlife supporting water quality and creating pleasant spaces for people to enjoy.
Conservation Volunteers experienced team leaders guide the programme and aim to teach volunteers about all aspects of conservation, including plant identification and planting techniques.
Join our community weeding day, bring all the family and share a delicious morning tea.
Phone 0800 56 76 86 or email email@example.com to book.
Join this project
There are currently no upcoming dates for this project.Find another project
About us
Conservation Volunteers New Zealand is New Zealand's leading conservation volunteer organisation, founded in 2006. We offer conservation programs across New Zealand which enable volunteers to protect, preserve and restore the environment. Projects take place in urban, regional and remote areas, and include tree planting, seed collection, weed control, flora and fauna surveys, building tracks and trails, fencing, and heritage restoration. See below for details of one of our conservation projects, or search for projects near you.
Contact us
For more information, or for help with your booking, please contact the Eden Terrace office on 00 64 9 300 7320 or email email@example.com


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Celebrating 20 years of competing in the Formula Student competition, the University of Birmingham's official team, UBRacing is preparing for this year's race season. The competition, which is organised in the UK by IMechE, the Institution of Mechanical Engineers, is all about building future engineering talent by designing and producing a single-seater racing car. As part of its YES (Young Engineers Support) programme, igus has backed the UBRacing team for several years with free engineering advice and products.
Charles Hodgson, Team Principal of UBRacing says: "Most of the members are Mechanical Engineering undergraduates; however, the team is not restricted only to engineering students. This is because the competition is based around running the team as a successful business, as well as producing a car that performs well under static and dynamic tests." Hodgson estimates that it costs £30,000 a year to run the project – all of which is funded through sponsorship and support from businesses.
This year, igus engineering plastic bearing products are being used in the car's steering rack, pedal box and for the anti-roll bar bushing. These tribologically optimised plastic materials are self-lubricating, meaning they require no maintenance. They are insensitive to dust and dirt and, depending on the material selected, are resistant to high temperatures, chemicals and moisture. Not only are they lighter than their metal counterparts, which is a decisive factor for choice but through intensive testing at its dry-tech test lab, igus can accurately predict the service life for any given application.
In the steering rack of this year's car, a drylin R press fit bearing is used at each end of the steering shaft. A drylin R standard liner, which features a long open design, is used in the centre to align the shaft as well as acting as a bearing. Hodgson explains: "Not only is this material extremely wear-resistant, it effectively dampens radial movement of the steering rack and thereby reduces vibration in the steering wheel."
In the pedal box, the engineering students developed a new design that enables the position of the pedals to move forward and backwards to suit the driver. For this, they selected two drylin T low-profile linear guides, which are easily adjustable. The rails and carriages are made of hard anodised aluminium, making the system resilient to high shock loads, as well as being lightweight and corrosion resistant.
Hodgson explains: "As we use different drivers for different events, this is very useful, and also is a feature that Design Event Judges liked, as the static events view the car as a business venture. This means that by having an adjustable pedal box, we can argue that we have a wider potential customer base and a more ergonomic vehicle."
The engineering team are also using iglidur P210 and iglidur J350 bar stock for the car's anti-roll bar bushings. These are necessary to allow the anti-roll bars to move freely, and are turned by the students to the correct size and shape for the car.
Matthew Aldridge, managing director of igus says: "We wish UBRacing good luck for the upcoming season. With the backing of many engineering companies across the UK, I am convinced the team will impress the jury with its ingenuity, thus bolstering the engineering faculty at the University of Birmingham."
More information about igus products can be found at www.igus.co.uk.


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Using competitive intelligence strategies and tools will be the key to launching successful email marketing campaigns in 2010, according to a new white paper from Compete. In the white paper "Five Simple Steps to Online Marketing Success," Compete recommends that marketers take the five following steps to integrate competitive marketing into their online campaigns:
1. Know the Competition: First, Compete advises email marketers to create a list of competitors in their space and identify the specific reasons each poses a competitive threat. After identifying their competitive set, marketers are advised to dig into metrics (i.e. unique visitors, page views, time on site, average stay, and pages per visit) and figure out their standing in the ones that matter most. All of these will give marketers a sense of real norms for their competitive landscape, thus allowing them to make logical business decisions and maximize ROI.
2. Cover Search Marketing Bases: Increase search traffic and campaign performance through analysis of competitors' search marketing trends and keywords. In addition, using local web analytics tools, marketers can see what keywords are sending traffic to their sites, how much of that traffic is paid as compared to natural, and what percentage of traffic the individual search engines contribute to a site overall. Through optimization and testing of paid search campaigns, SEO keyword research, and content creation, marketers can maximize conversions and increase search ROI. However, optimization and testing are not guaranteed to provide beneficial results. Competitive search analytics tools let marketers quickly gain insights into your competitors' search strategy so you can capitalize on their success.
3. Copying is a Sign of Flattery: Identify what websites are sending competitors' traffic and get in on the action. Competition for web traffic will continue to grow as more everyday activities move online. Just like there are a few keywords that drive most of the traffic to a site (the head) and thousands of other keywords that drive a little (the long tail), traffic to websites works much in the same way. There are millions of websites out there, however only a small percentage account for the bulk of traffic. By analyzing referral (upstream) and destination (downstream) traffic for their competitive sets, marketers can easily identify new affiliate websites, business relationships, and link-building opportunities.
4. Fix Your Leaky Bucket: Local web analytics tools will let marketers identify which websites are sending traffic to their sites. Based on page views, bounce rates, and conversion rates, they can easily identify which websites deliver the most benefit. Thinking of a website as a bucket, using various marketing tactics, marketers can scoop up site visitors that may be interested in their products or services. Then by creating conversion funnels, they can attempt to lead users to perform a specific action. Using destination or downstream traffic tools, marketers can easily see where their users go when they leave the site. Are they going directly to a competitor, a search engine, or back to their favorite social network? Maybe they are searching for coupons on their favorite deal sites or conducting research before they decide to purchase your products or services. By regularly performing a destination traffic report on their websites, marketers can easily find opportunities to quickly 'patch the holes' in their 'leaky buckets.'
5. Stay on Top: Marketers should monitor, set benchmarks, and realize how their site enhancements and marketing strategies impact their competitors. In order to stay on track and continue to grow their business, marketers need an online marketing strategy that can adjust to ever-changing economic, technological, and social environments. Incorporating competitive intelligence into that marketing strategy can give them the critical information they need to minimize risk and ensure success. Marketers should monitor their competitive set and use competitive intelligence tools on a regular basis. They will find much of the information they collect to be critical in making decisions about their overall marketing strategies. Then, they should set benchmarks and monitor changes across their entire competitive sets.


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Unfortunately, this workshop became unavailable due to the coronavirus fear.
Hope we can organise another workshop a our next pop-up in late-June!
Chakabuki is a matcha tasting game that was popular among the intellectual in Kyoto between the late Kamakura period (1185-1333) and the middle of the Muromachi period (1338-1573). In our version, Wendy will introduce three different types of matcha which participants will taste. The matcha will then be shuffled and you will do a second round of blind tasting, and attempt to guess the type of matcha.
You can choose to taste the tea the traditional way -sharing from one matcha bowl- or choose to have their own teacup for the duration of the tasting. Japanese sweets will also be provided to complement the tea.
About Matcha
Matcha is a fine powdered green tea which is harvested and made under strict conditions to maintain high quality. While one serving of matcha (fine powdered green tea) has much less caffeine than coffee, it provides a less jittery, more sustained energy boost -with no crash at the end. L-Theanine also improves focus and helps you concentrate.
Date, time & location
5 April, 11am-12pm
Cubby Space, 114 George St Redfern NSW 2016
Easily accessible by train. Free street parking is also available in the area.
What to bring
Nothing, we'll provide everything!
What you'll take home
- Three different types of matcha to taste.
- Japanese sweets to complement the tea.
Cancellations are possible up to 72 hours (3 days) before the session. Please e-mail info[at]simply-native[dot]jp


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Euronda Monoart Saliva Ejectors 15 Cm Blue 100/pk - EM15/B (Web Special Offer)
In stock
was ₹220.00 Special Price ₹205.00
(Price Per Pack Inclusive of GST)
Disposable flexible saliva ejector made of non-toxic transparent PVC. Integrated mettalic wire for the excellent maintainence of the set angle. Rounded shape fixed tip, ideal for work on irritated mucous. Size Diameter 6.5 mm. Medical Device Class II A. Pack of 100 Pcs of 12.5 cm &15 cm Length. Also known as Suctip Tips
Write Your Own Review
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Dickinson T-1000 Straight Pull Bolt Action Shotguns represent a change in the way we think of modern sporting arms.
Designed from the ground up to meet Australian shooter demands, these shotguns allow for faster follow up shots, and their increased capacity goes well beyond that of a standard over and under. Further, Dickinson T-1000's price-point is incredibly reasonable, meaning you are getting an excellent quality gun at a very affordable price.
Its straight pull design allows the user to simply pull the bolt handle backwards allowing for fast ejection of spent shells, quick reloading from the magazine tube, and re-cocking of the firing pin. Once the bolt handle is let go by the shooter, it feeds the next round into the chamber ready to be fired.
Dickinson's T1000 Timber features Turkish Walnut stock and forearm and is perfect for those who prefer the feel and look of a more traditional firearm.
20 Gauge scaled frame straight pull shotgun
28" Barrels
Turkish Walnut Stock
5 x Mobil Chokes
3" Chamber
Adjustable shims included
4 + 1 Capacity


text: January 14th, 2017. Yaaaaay another trip to Singapore. I always loved Singapore. Such an organized place. So when Darius and Gaby showed off their tickets, I bought my ticket in a flash. Singapore, here we come! And first coffee shop, Dutch Colony. Located in UE Square, at first we thought they have outdoor seats. Turned out,Continue reading "[SINGAPORE] Dutch Colony Coffee Co. at UE Square"