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Dumpster Rental in Warwick MA
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We are always available to help
Simply give us a call and we will answer any questions you may have about the Warwick dumpster rental procedure, allowed materials, size you may need, etc.
Next-Day delivery of your dumpster
Our roll off containers can usually be delivered in Warwick the day after you place your order. Make sure to call us early to ensure timely delivery.
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How Long Can I Rent a Dumpster For?
The total amount of time that you will need to rent a dumpster in Warwick ordinarily depends on the type of project you are working on. A small endeavor, for example a cellar clean out, will probably take a few days to finish while larger projects, like building a new house, could take several months.
Most firms in Warwick are happy to adjust their schedules to suit your needs. Keep in your mind, however, that the the more time you keep the dumpster, the more you'll need to pay for it.
When you contact firms in Warwick, ask them how long their durations are. Many will allow you alternatives such as several days or one week, but there are typically longer durations available, also.
You also ought to ask how much the firms bill for extra time. That way, you know how much it costs to maintain the dumpster for a couple of extra days if needed.
What if I want my dumpster in Warwick picked up early?
When you make arrangements to rent a dumpster in Warwick, part of your rental agreement contains a stated duration of time you're permitted to use the container. You normally base this time on the length of time you think your project might take. The larger the project, the the more time you'll need the dumpster. Most firms in Warwick give you a rate for a certain amount of days. Should you exceed that quantity of days, you will pay an extra fee daily. If the project goes more quickly than expected, you may be finished with the dumpster earlier than you anticipated.
If this is true, give the dumpster company a call and they will probably come pick your container up early; this will enable them to rent it to someone else more immediately. You generally WOn't get a reduction on your own rate if you ask for early pick up. Your rental fee includes 7 days (or whatever your term is), whether you use them all or not.
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Can I haggle to get a better price?
Dumpster rental companies usually have set prices, but the fine art of negotiation is always in play. In case you want to dicker on the price, call around to other companies first so you understand what the going rental rate is. When you're talking to the business you would like to utilize, merely mention other prices which are better than theirs. Some companies WOn't only fit that lower cost, they will actually beat it to satisfy their customers.
You can also ask about discounts when you're renting a dumpster in Warwick. Some companies will supply special discounts to active members of the military, veterans, seniors, members of the local Chamber of Commerce and much more. It really never hurts to ask; you can sometimes save up to 10 percent or more with this system.
You can also save on the cost by asking about the simplest way to prevent additional expenses (such as tipping fees or overage charges) and making sure you order the right size container; you do not desire to pay for more container than you actually desire.
20 yard dumpster dimensions in Warwick
A 20 yard dumpster can hold about 20 cubic yards of waste or debris. Standard dimensions for a 20 yard container are about 22 feet long by 8 feet wide by 4.5 feet high. With these dimensions, a 20 yard dumpster can hold about 10 pickup truck loads of debris and waste. This implies that the 20-yarder is a standard size for jobs that call for clean-up from bigger endeavors. Because of its compact size that still has capacity for a great volume of debris, a 20 yard container is one of typically the most popular dumpster sizes for home jobs. Examples of what can fit in a 20 yard container comprise:
- Clean-Up from a cellar, attic or garage
- Flooring and carpeting removal from a sizable house
- 300 to 400 square feet of deck removal
- 2,500 to 3,000 square feet of shingle removal from a single layer roof
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City regulations on in Warwick
Most cities or municipalities don't have many regulations regarding in Warwick as long as you keep the dumpster completely on your own property during the rental period. Should you have to put your container on the road at all, you will likely need to obtain a license from the appropriate building permit office in your town.
Most companies in Warwick will take care of securing this license for you if you rent from them. Ensure that if you're planning to place the dumpster on the road, the firm has made the proper arrangements. You should also ensure that you get the license in a timely manner and at the correct cost. In case you thought the dumpster company was getting a license and they did not, you will be the person who will have to pay the fine that's issued by the authorities.
Reasons to Work With a Flat Rate Service when Renting a Dumpster
Dumpster rental businesses that charge flat rates are frequently the most effective options for contractors and home owners. When you take advantage of a company that bills a flat rate, you can expect at least two benefits.Avert Hidden Charges
Paying a flat rate usually means that you simply get to avoid any hidden fees and charges. Businesses that don't charge flat fees may include extra charges for basic services like dropping off the dumpster. Keep in mind, nevertheless, that you still may have to pay extra in case you wish to include certain things and materials in the dumpster.Prepare Your Payment in Advance
Having a flat rate also means you can prepare your payment in advance. This is especially useful when you need another person to make the payment for you. When you know the exact quantity, you can write a check in advance. Then, anyone can pay the rental company when its driver drops off the dumpster.
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Choosing the top dumpster for your job size
Choosing the top dumpster for your job is an important aspect of in Warwick. Should you choose a dumpster that's too small, you will not have enough room for your debris and waste, which means you'll have to schedule additional excursions. In the event that you choose one that's too big, you'll save time, but you'll squander cash.
Should you call a company in Warwick and describe the job for which you need a dumpster, they can urge the best size. Their years of experience mean that they often get it just about right. A 10-yard dumpster usually functions well for medium-sized cleaning projects and modest remodeling jobs. A 20-yard dumpster is the best choice for big residence cleaning projects and medium-sized renovation projects, while a 30-yard dumpster has higher walls that are ideal for a home cleanout or remodeling jobs on a sizable house. 40-yard dumpsters are massively big and are used just on the biggest projects like new building.
Determining Where to Place Your Dumpster
Determining where to place your dumpster can have a huge impact on how quickly you complete jobs. The most efficient option would be to pick a location that's close to the worksite. It's important, nevertheless, to contemplate whether this location is a safe choice. Make sure the area is free of obstructions that could trip people while they take heavy debris.
Many people choose to set dumpsters in their own driveways. This is a handy choice because it usually means you can avoid requesting the city for a license or permit. If you must set the dumpster on the road, then you definitely should get in touch with your local government to ask whether you are required to get a permit. Although many municipalities will let people keep dumpsters on the road for short levels of time, others are going to request that you fill out some paperwork. Following these rules will help you stay away from fines that will make your project more costly.
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Dumpster Rental Companies Near Warwick
|Company Name
|The Trash Guy
|(508) 344-2080
|Wolpert Disposal Inc
|(978) 463-5400
|Brunnett Rubbish Removal
|(508) 892-9803
|Murray & Sons Waste
|(978) 386-7749
|Ramco Survey Stakes Inc DBE WBE SOMWBA Certified
|(508) 580-3400
|Hiltz Waste Disposal
|(978) 283-3335
|Mass Portering Services Inc
|(508) 473-5393
|Cavossa Disposal Corporation
|(508) 563-5070
|Boston Children's Museum
|(617) 426-6500
|C J Rubbish Removal Inc
|(508) 947-6420
Our Service Area
Zip Codes in Warwick01378
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Dumpster Sizes Available Warwick
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10 Yard
Great for small projects
- 12 feet long
- 8 feet wide
- 4 feet tall
20 Yard
For moderate sized cleanouts
- 22 feet long
- 8 feet wide
- 4.5 feet tall
30 Yard
All around good dumpster size
- 22 foot long
- 8 feet wide
- 6 feet tall
40 Yard
For the largest projects
- 22 foot long
- 8 feet wide
- 8 feet tall
*Dimensions & availability may vary by location. Call to confirm.
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Topological insulators are a unique class of materials characterized by a Dirac cone state of helical Dirac fermions in the middle of a bulk gap. When the thickness of a three-dimensional topological insulator is reduced, however, the interaction between opposing surface states opens a gap that removes the helical Dirac cone, converting the material back to a normal system of ordinary fermions. Here we demonstrate, using density function theory calculations and experiments, that it is possible to create helical Dirac fermion state by interfacing two gapped films—a single bilayer Bi grown on a single quintuple layer Bi2Se3 or Bi2Te3. These extrinsic helical Dirac fermions emerge in predominantly Bi bilayer states, which are created by a giant Rashba effect with a coupling constant of ~4 eV·Å due to interfacial charge transfer. Our results suggest that this approach is a promising means to engineer topological insulator states on non-metallic surfaces.
Topological insulators (TIs) have attracted a great deal of recent interest as a new class of materials1,2,3,4,5,6,7,8,9. One unique property of TIs is its electronic structure characterized by the helical Dirac cone states residing in the middle of a bulk insulating gap. Charge carriers in such Dirac states are helical Dirac fermions (HDFs), which, different from ordinary fermions, are massless relativistic particles with their spin locked to their momentum ideally in perpendicular direction. On one hand, the HDFs are expected to give rise to a range of fundamentally new physical phenomena, such as anomalous half-integer quantum Hall effect10,11, Majorana Fermions12 and fractionally charged quantum particles13. On the other hand, the spin transport of HDFs is protected against back scattering by time-reversal symmetry, which affords a promising paradigm of spintronic devices.
So far, the HDFs are considered to be an intrinsic property of TIs, which only exist in TIs with sufficient size. If the dimension of three-dimentional TIs is reduced, the coupling between the surface states coupled with quantum confinement effect will open an energy gap, eliminating the HDF states, that is, the linear Dirac bands of HDFs revert to the parabolic conventional bands of normal fermions upon gap opening14,15,16. For example, when the thickness of Bi2Se3 (or Bi2Te3), two well-known three-dimensional TIs, is reduced to less than six quintuple layers (QLs), a gap opens14,15,16. While the ultrathin Bi (111) films of less than four bilayers (BLs), a two-dimensional TI system, is characterized with a finite gap17,18,19,20. Therefore, the common expectation is that the HDFs cannot survive in the gapped systems.
Here we report the discovery of extrinsic formation of HDFs by interfacing two gapped thin films: a single BL Bi (111) film grown on a single QL Bi2Se3 or Bi2Te3 substrate. Using density function theory (DFT) band calculations, we predict the existence of helical Dirac cone in such supposedly ordinary fermion systems and the prediction is directly confirmed by experiment. Further theoretical analysis shows that the extrinsically created helical Dirac cone consists of predominantly Bi bilayer states. It is induced by a giant Rashba effect of band splitting with a coupling constant up to ~4 eV Å, resulting from the internal electric field due to interfacial charge transfer. Our findings provide a promising new method to manipulate the electronic and topological states by interface engineering.
Construction of two gapped systems
Our idea of interfacing two gapped films of single BL Bi (111) film and single QL Bi2Se3 or Bi2Te3 is partly motivated by existing knowledge of growing Bi film on different substrates. It is known that when Bi grown on metal21,22 or semiconductor substrates (for example, Si, Ge)23,24,25, an extrinsic helical Dirac surface state can be created by the substrate induced spin-splitting of Bi bands, that is, the Rashba effect. However, generally there exist strong interactions between the Bi and the substrate leading to strong hybridization of surface and bulk states, and additionally metal substrate is undesirable for device applications. Recent experiments have grown Bi (111) bilayer on TI Bi2Te3 (refs 26, 27) and Bi2Se3, which also see extrinsic formation of the helical Dirac states from Bi. However, the problem remains that there exists the intrinsic Dirac state and other bulk states of Bi2Te3 substrate that can hybridize with the extrinsic surface Dirac state of Bi BL27. Therefore, one needs to find a suitable gapped substrate for growing Bi that will avoid strong hybridization between the extrinsic Bi Dirac states and substrate states, so as to better isolate surface Dirac transport. In this regard, growing Bi bilayer on a gapped 1QL Bi2Te3 (or Bi2Se3) substrate versus on a semimetal thick (>6 QL) Bi2Te3 (or Bi2Se3) substrate makes a significant difference. Further, experimentally growing high quality 1QL Bi2Te3 (or Bi2Se3) film turns out to be much harder than thick films, as we discuss below.
DFT band structures
A single BL Bi (111) film is predicted to be a gapped two-dimensional TI17,18,19,20. Our calculations show that at the equilibrium substrate lattice constant of Bi2Se3 and Bi2Te3, the strained Bi (111) film has an energy gap of ~0.17 eV (Fig. 1a) and ~0.44 eV (Supplementary Fig. S1a), respectively. On the other hand, Bi2Se3 and Bi2Te3 are well-known three-dimentional TIs with a single helical Dirac cone below Fermi level. However, when their thickness is reduced to <6 QL, a finite energy gap opens removing the Dirac cone. As shown in Fig. 1b and Supplementary Fig. S1b, we can clearly see an energy gap in 1QL Bi2Se3 (~0.5 eV) and Bi2Te3 (~0.3 eV), which are consistent with previous works15,16. After 1BL Bi (111) is deposited onto 1QL Bi2Se3 (or Bi2Te3), the band structures are found to change dramatically. Most surprisingly, the gap vanishes as a linear dispersive band emerges around the Г point to form the Dirac cone, marked with 'D' in Fig. 1c and Supplementary Fig. S1c,d. For the Bi/Bi2Se3 (Fig. 1c), the Dirac point locates at ~0.1 eV below the Femi level with a Fermi velocity (VF) ~5.3 × 105 m s−1; for the Bi/Bi2Te3 (Supplementary Fig. S1c,d), the Dirac point locates at ~0.2 eV below the Femi level with a VF~4.5 × 105 m s−1. We note that the extrinsic Dirac point formed in our system is not perfect as the second derivative of E(k) doesn't exactly vanish. However, the E(k) is almost linear with spin-momentum locking property, having a very large Fermi velocity comparable to that in graphene or other TIs. Therefore, from charge and spin transport point of view, our system works equivalently well for spintronics device applications.
Angle-resolved photoemission spectroscopy band structures
Our DFT predictions are directly confirmed by experiments, as shown in Fig. 2. A single BL Bi (111) is grown on the (111)-oriented 1QL Bi2Se3 substrates, which were grown first on graphene prepared on SiC wafer28. We found that growth of high quality ultrathin film of 1QL Bi2Se3 or Bi2Te3 turned out to be much harder than growth of thick film of multi-QLs. So far, we only attained high quality of 1QL Bi2Se3 film to our satisfaction, but not for 1QL Bi2Te3. The thickness and quality of the films are monitored by in situ reflection high-energy electron diffraction and scanning tunnelling microscopy (STM). The electronic bands are measured directly by angle-resolved photoemission spectroscopy (ARPES). In Fig. 2a, an energy gap is observed for the bare 1QL Bi2Se3. Bi can grow epitaxial with a unit of BL along (111) orientation on Bi2Se3. After deposition of a single BL Bi (111), the spectra are dramatically changed and a Dirac cone clearly appears around the Γ point, as shown in Fig. 2b. The DFT bands calculated at the experimental graphene lattice constant (green dashed lines) are overlaid with the ARPES spectra along high symmetric directions and the agreement between the theory and experiment is very good. In order to match experimental data, the Fermi level of DFT bands is slightly shifted. The Dirac cone is isotropic. Fig. 2d presents the high resolution ARPES spectra near the Dirac cone and corresponding momentum distribution curves. The linearly dispersive bands of the Dirac cone are clearly resolved. The Dirac point is about 0.07 eV below Fermi level estimated from the crossing point of the linearly dispersive bands (green dotted line). The VF of the Dirac cone is ~6 × 105 m s−1, which is the same as that of bare Bi2Se3.
Extrinsic helical Dirac states
We have also confirmed the helical properties of the newly formed extrinsic Dirac cones in the interfaced systems of a single BL Bi (111) and 1QL Bi2Se3 (or Bi2Te3), which are individually gapped materials. HDFs are characterized by the spin-momentum locking relations29: (i) the spin direction is perpendicular to the momentum direction; (ii) the spins have the opposite directions at the inverse momenta. We have calculated three spin components of the Bloch state in the Brillouin zone, as shown in Fig. 3. Figure 3a shows the zoom-in band structure around the Dirac cone for the Bi/Bi2Se3 system, indicating two equal-energy cuts (circles) above and below the Г point with k=0.04 Å−1 (radius of circle). The in-plane spin projections along the upper and lower circles are plotted in Fig. 3c, respectively. The spins point clockwise around the upper circle, but counterclockwise around the lower circle, and they are in opposite directions at the inverse momenta. In addition, the spins are not completely in-plane, and their out-of-plane projections are plotted in Fig. 3e, which oscillate periodically around circle with a period of 120° (reflecting the threefold rotational symmetry) and have the opposite phase in the upper and lower circles. Thus, as the electrons trace the circle in momentum space, their spins lie almost in the plane of the circle, but wobble above and below the plane periodically. The finite out-of-plane spin-component is due to the warping effect of the Dirac cone (see Fig. 3a), which has not a perfect linear dispersion. The six nodal points in the out-of-plane wobbling motion (Fig. 3e) correspond to high-symmetry Г-M directions. We also calculated the angle (α) between the electron spin and momentum direction, as shown in Fig. 3f. α is very small, <0.3° and 0.1° in the upper and lower circle, respectively, indicating that spins are almost perpendicular to their momenta. All these features demonstrate the spin-momentum locking property of the helical Dirac states. The same results and conclusions are drawn for the Bi/Bi2Te3 system, as shown in Supplementary Fig. S2.
Next, we explain where the Dirac cone states come from, the 1BL Bi or 1QL Bi2Se3 (or Bi2Te3)? Previous studies18 showed that the Bi (111) film represents a special class of system having an intermediate inter-bilayer coupling strength, which has a significant influence on its topological property. At equilibrium, the interfacial distance (d) between Bi BL and Bi2Se3 QL is ~3 Å and the interface energy is ~0.16 eV per unit cell, which are noticeably larger than the typical values of van der Waals bond but smaller than those of typical chemical bond. To gain some insight about the influence of the interfacial coupling on the helical spin states, we have performed a set of model DFT calculations by artificially increasing the interfacial distance between the Bi BL and Bi2Se3 QL to gradually tune the interface coupling strength18, as shown in Fig. 4. At a large interfacial distance (for example, d~6 Å in Fig. 4a), without the interfacial coupling, the band structure would be a simple superposition of the bare Bi BL and Bi2Se3 QL bands. However, we observe a slight band splitting in the double-degenerated Bi and Bi2Se3 band. With the decreasing interfacial distance, the increased interfacial coupling continues to further split and reshape the bands, leading eventually to the formation of helical Dirac cone. By analysing the spectral components of Dirac cone states during this process, we found that the Dirac cone is predominantly coming from the Bi BL, with ~95% spectral weight of Bi BL states at the equilibrium distance, as shown in Fig. 4c. Similar results are found for the interface between Bi BL and Bi2Te3 QL, with ~90% Bi BL states in the helical Dirac cone at the equilibrium distance, as shown in Supplementary Fig. S3a–c.
Lastly, we will address how the Dirac cone states are formed. From the above calculations and analyses, we learnt that the extrinsic HDFs originate from the Bi BL, while the QL of Bi2Se3 (or Bi2Te3) substrate provides possibly a triggering mechanism that induces the Dirac cone states in Bi BL. We also know that Bi (111) BL has a strong spin-orbit coupling, and by itself its bands are double-degenerate conserving the inversion symmetry. Deposition of Bi BL on Bi2Se3 (or Bi2Te3) will break such symmetry, and hence lift the band degeneracy. However, this effect of symmetry breaking is limited, likely insufficient to induce a band splitting and reshaping as dramatic as we have observed. To further understand the interaction between the Bi BL and Bi2Se3 (or Bi2Te3), we calculated the differential charge density at the interface, defined as ρdiff=ρBL+QL−ρBL−ρQL, as shown in Fig. 4d (see also Supplementary Fig. S3d for Bi/Bi2Te3). Clearly, a substantial charge transfer at the interface has occurred. The Bi BL acts as a donor and the Bi2Se3 (or Bi2Te3) as an acceptor, with the electrons transferring from the former to the latter. This charge transfer generates a large internal electric field at the interface region, with a field direction pointing from the Bi BL to the Bi2Se3 (or Bi2Te3), and field intensity estimated as high as ~1 V/Å. Thus, we propose this phenomenon is very similar to the external electric field (or band bending) effect that induces Rashba band splitting in the surface state of TIs30,31,32. We estimated the Rashba coupling constant (using the two-dimentional free electron gas model) from the calculated band splitting at the equilibrium structures, which is ~4 eV·Å. Therefore, the HDFs are extrinsically created by a giant Rashba effect due to the interfacial charge transfer.
To further support the charge transfer induced Rashba effect is the dominated factor for realizing the extrinsic helical Dirac states, we also studied the band structure for Bi BL on 1QL In2Se3 and 5-layer Cu (111) substrate, as shown in Supplementary Figs S4 and S5, respectively. A clearly charge transfer between the Bi BL and these non-TI substrates (Supplementary Figs. S4i and S5i) can be observed in both cases (one semiconductor and one metal), and the similar Dirac cone states are also generated. However, the Bi BL become metallic at the In2Se3 lattice constant, and the Cu (111) substrate is also metallic. Thus, comparing to Bi/Bi2Se3 and Bi/Bi2Te3 system, these Dirac cone states are not within the gapped region of Bi/In2Se3 and Bi/Cu. The previous studies for Bi grown on Si (111) only showed the monomer or trimer Bi configuration on the substrate, which cannot maintain the intrinsic structure of the Bi BL.
Calculation method
DFT calculations for a single BL Bi (111) on a single QL Bi2Se3 and Bi2Te3 are carried out in the framework of the Perdew-Burke-Ernzerhof-type generalized gradient approximation using VASP package33. The experimental bulk lattice constants of the substrate are used (a=4.138 Å for Bi2Se3 and a=4.386 Å for Bi2Te3), and the Bi BL is strained to match the substrate lattice constant. All calculations are performed with a plane-wave cutoff of 400 eV on an 11 × 11 × 1 Monkhorst-Pack k-point mesh, and the vacuum layer is over 20 Å thick to ensure decoupling between neighbouring slabs. During structural relaxation, all the atoms are allowed to relax until the forces are smaller than 0.01 eV/Å. To reproduce the ARPES band for Bi/Bi2Se3 in Fig. 2, we use a larger lattice constant a=4.37 Å, which can match the graphene/SiC wafer in the experiment.
Experiment method
Flat Bi2Se3 single QL films is grown by molecular beam epitaxy method on graphene/SiC wafer and on highly ordered pyrolytic graphite substrates. Bi films are deposited on Bi2Se3 at 200 K and then annealed at room temperature. The thickness of Bi2Se3 and Bi films is monitored by reflection high-energy electron diffraction oscillation and scanning tunnelling microscopy. The sample temperature is kept at 100 K during measurement. ARPES measurements are performed with in-lab He discharge lamp (He-I 21.2 eV). Energy resolution is better than 25 meV and angular resolution is better than 0.02 Å−1.
Additional information
How to cite this article: Wang, Z.F. et al. Creation of helical Dirac fermions by interfacing two gapped systems of ordinary fermions. Nat. Commun. 4:1384 doi: 10.1038/ncomms2387 (2013).
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The theoretical work was supported by US DOE-BES (Grant No. DE-FG02-04ER46027) and we thank the CHPC at University of Utah and NERSC for providing the computing resources. The experimental work was supported by National Basic Research Programme of China (Grant No. 2012CB927401, 2011CB921902, 2013CB921902, 2011CB922200), NSFC (Grant No. 91021002, 11174199, 11134008, 11274228), Shanghai Committee of Science and Technology, China (No. 11JC1405000, 11PJ1405200, 12JC1405300), Shanghai Municipal Education Commission (11ZZ17) and SRF for ROCS, SEM. Z.F.W. acknowledges additional support from ARL (Cooperative Agreement No. W911NF-12-2-0023). W.M.M. acknowledges additional support from NSF-MRSCE (Grant No. DMR-1121252). D.Q. acknowledges additional support from 'ShuGuang' project supported by Shanghai Municipal Education Commission and Shanghai Education Development Foundation and from Programme for Professor of Special Appointment (Eastern Scholar) at Shanghai Institutions of Higher Learning.
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Further reading
Topological edge states in high-temperature superconductiving FeSe/SrTiO3 films with Te substitution
Scientific Reports (2019)
Functionalized Thallium Antimony Films as Excellent Candidates for Large-Gap Quantum Spin Hall Insulator
Scientific Reports (2016)
Emergent phenomena induced by spin–orbit coupling at surfaces and interfaces
Nature (2016)
Topological proximity effect in a topological insulator hybrid
Nature Communications (2015)
Formation of quantum spin Hall state on Si surface and energy gap scaling with strength of spin orbit coupling
Scientific Reports (2015)
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Human Performance
Why I Quit Coaching Advisors
I have been coaching for a long time.
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text: I have had this quilt top "Vintage Vacation" done for a couple of years from a pattern that I designed. A friend of mine gave me the fabrics that her mom had from the 1970s. When it came to quilting, I thought a double line decorative zig-zag would be a fun choice as it resembles ric-rac to me.


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The latest receipts from HMRC published on the eve of the Budget show the taxman is on course to take a record £5.5 billion from people's estates this tax year, according to NFU Mutual.
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Individuals were hit with a £4.84 billion 'death tax' charge in the 2016/17 tax year, the latest official figures from HM Revenue & Customs (HMRC) show.
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Much fanfare has been made of the new inheritance tax (IHT) allowance for main homes, which will reduce IHT liability for many people when it is introduced in April.


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This question already has an answer here:
I need to check if the number has decimals. Since you can't do type checking for type float or a double I came up with the the following code.
$('#storePaymentForm').submit(function() {
var numberValue = document.getElementById("price").value;
if (numberValue % 1 != 0) {
return true;
else {
alert('U moet een bedrag invullen met twee nullen achter de commas!');
return false;
This code works fine when you enter a number like:
10.23 But when you enter
10.00 it returns false and shows the alert. I've tried several things, but I can't figure it out. Can anyone help me or point me in the right direction how I can check if the number has decimals. And make sure when a user enters
10.00 it returns true instead of false(which is the case right now). The input field is of type number.
The input field looks like this:
<input type="number" id="price" required name="price" min="0" value="0.00" step=".01">