![]() ![]() In all, Crest checked prices on 35 items that day and found that Crest beat or met prices at four "other" Wal-Mart Supercenters in 22 out of 35 items. But the Edmond Wal-Mart Supercenter was selling the mustard for 50 cents. Crest was selling the product for 88 cents. Oklahoma law prohibits selling products below cost if the intent is to injure a competitor or prevent fair competition.Ĭrest's executives said that according to their June 9 price survey, French's mustard sold for 88 cents at the Wal-Mart Supercenters in Moore and Norman and 97 cents at two Oklahoma City Wal-Mart Supercenters. "We deny very strongly that our pricing was intended to drive this supermarket or any other competitor out of business," Wertz said. ![]() In addition, Wertz said that such comparison shopping is a standard retail practice long used by Wal-Mart and its competitors, but he also said it would not be a big deal to be asked to leave while comparison shopping. "Anybody in the retail industry who knows David Glass knows him to be a very conservative and even-tempered executive." "With respect to the comments about David Glass, this is a completely fabricated assertion," Wertz said. "The Store Manager or other responsible Wal-Mart Management shall request that any employee of a competitor who is recording (price) data inside our store immediately stop the recording or leave our premises," the handbook says. Meyers and Rupert have obtained a Wal-Mart employee handbook that instructs managers to kick out competitors who enter Wal-Mart stores to record their prices. Glass, who succeeded Wal-Mart founder Sam Walton, stepped down as president and CEO in January but remains chairman of Wal-Mart's executive committee of directors. The lawsuit does not reveal the source of its allegation concerning Glass. Glass ordered the Edmond Supercenter to obtain revenge by dropping its prices even below cost if necessary to drive Crest out of business," the lawsuit alleges. Glass was personally offended that he was 'kicked out' of Crest (even though he was subsequently invited to stay), and that Mr. The lawsuit says that a Crest assistant manager asked the people to leave, suspecting that they were snooping for Wal-Mart, but that a senior manager told them they could stay if they wished. Crest alleges that the group was using a hand-held scanning device to record Crest's prices of various items. This is an unfortunate attempt to generate publicity."Īccording to the lawsuit, David Glass, the former president and chief executive officer of Wal-Mart, along with several other Wal-Mart personnel, visited Crest Foods on May 23, just six days after the opening of the Edmond Wal-Mart Supercenter. "We engage in fair competition and try to give our customers the best value," Wertz said. "It's not the typical story of the mom-and-pop store getting underpriced by Wal-Mart and complaining," Rupert said.īill Wertz, a Wal-Mart spokesman, denied Crest's accusations. They claim Wal-Mart has a vendetta against Crest. ![]() ![]() As a result, Crest filed a lawsuit Tuesday in federal court in Oklahoma City against the Bentonville, Ark., retailer seeking millions of dollars in damages.īut it's about more than competition, said Kent Meyers and Tony Rupert, the Crowe and Dunlevy attorneys who are arguing the case. Wal-Mart is known for its competitive prices, but an Oklahoma City grocer claims the retail titan has taken a good thing too far.Ĭrest Food claims that the Edmond Wal-Mart Supercenter has engaged in "predatory pricing" to drive the Edmond Crest Foods store out of business. ![]()
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![]() Sinéad O'Connor: Irish Singer and 'Nothing Compares' Subject Dead at 56 ‘Nothing Compares’ Makes A Convincing Case For The Late Sinead O’Connor’s Canonization Tori Kelly Shares Positive Update After Her Recent Hospitalization, but Reveals "There Are Still Some Things to Uncover" The 'Victoria's Secret Fashion Show' Returns: Reimagined "Fashion Event" And Documentary Special to Stream on Prime Video Stream It Or Skip It: 'After the Bite' on HBO and Max, a Profound, Fascinating Documentary About the Relationship Between Humans and Sharks Stream It Or Skip It: ‘The Lady of Silence: The Mataviejitas Murders’ on Netflix, an Occasionally Lascivious True Crime Documentary Jamie Lee Curtis Opens up About Her Addiction to Opiates, Says She'd Be "Dead" if Fentanyl Was "as Easily Available as It Is Today on the Street" 'Oppenheimer' IMAX 70mm Tickets Are Going For Upwards Of $500 Sinead O'Connor's Refusal To Be Shamed For What She Believed In Made Her The Ideal Avatar For Neil Jordan's Uniquely Irish WorldviewĮlizabeth Banks Would Be “Thrilled” To Do ‘Cocaine Bear 2’ ‘The Beanie Bubble’ True Story: How Accurate Is the Zach Galfianakis Movie About Ty Warner? 'American Pie' Star Seann William Scott Reveals He Only Made $8,000 For Playing Stifler: "Ended Up Having to Work at the LA Zoo as a Churro Guy" 'Minx' Season 2 Episode 2 Recap: "'Deep Throat' Is Missing!"ħ Movies Like 'Barbie' If You Find Yourself In Need Of A Dose Of Girl Power ![]() Stream It Or Skip It: ‘Smoking Causes Coughing’ on Hulu, An Crazy Comic Caper with Atypical Avengers ![]() ![]() ![]() Inside nested loop or conditional statements also become nested. Remaining code and become nested inside the sections in the remaining code. Within the loop or conditional statement are independent from the sections in the Statement (if those lines do not already contain a section break). MATLAB adds section breaks at the lines containing the start and end of the In the Editor, if you add a section break within a loop or conditional statement Behavior of Sections in Loops and Conditional Statements Script, you can run only the sections that are before the local functionĭefinitions. When running individual sections in a live Script, MATLAB adds a section break before the first local function definition and Inside local functions are not supported. In the Live Editor, you cannot add section breaks inside a function. Statement, MATLAB behaves as if the end of the function occurs immediately before the m ), you can enhance the readability of the published documents by adding markup to the comments within the files. If you do not end the function with an end When publishing your MATLAB code files (. In the Editor, if you add a section break within a function, MATLAB inserts section breaks at the function declaration and at the functionĮnd statement. MATLAB runs the section after every click. Then, click one of the operator buttons to add to, subtract from, multiply, orĭivide the selected value in your section. In the dialog box that appears, specify a step valueįor addition and subtraction or a scale value for multiplication and division. Next, right-click and select Increment Value and To adjust a numeric value, select the value or place your cursor next to the Workflow can help you fine-tune and experiment with your code. Values within a section, rerunning that section after every change. In the Editor, you can increment, decrement, multiply, or divide numeric Information, see Debug MATLAB Code Files. In functionsĪvailable only when evaluation is paused. In the Live Editor,Īvailable for all code, whether it is saved or not. MATLAB continues running until the end of the file isĪvailable only for code that has been saved. Run to a specific line of code and pause. ![]() Run the code in the selected section, and then run all the code Run the code in the selected section, and then move to the next This table describes different ways to run your code. When running individual sections, MATLAB does not save your file and the file does not have to be on your To run a section individually, it mustĬontain all the values it requires, or the values must exist in the MATLAB workspace. Running all of the code in the file at once. You can run your code file by either running each section individually or by The gray area to the left of your code and clear the Show Run Section To hide one or more of the margins, right-click This minimizes the grayĪrea to the left of your code. The Run Section, Run to Here, and Code Folding margins. To maximize the space available for editing code in the Editor, you can hide For more information about when MATLAB might add a section break, see Behavior of Sections in FunctionsĪnd Behavior of Sections in Loops and Conditional Statements. ![]() You cannot remove sections breaks added by MATLAB. ![]() ![]() ![]() ![]() In other words, if the electric field is confined to the depletion region, then the net charge in Region II must be zero, and hence the negative charge and the positive charge must be equal. This equation makes physical sense since it states that the total charge on one side of the junction must be the same as the total charge on the other. Putting x = 0 in the above equation for electric field and setting the two values of E equal to each other gives: N Ax p = N Dx n. Further, we know that the electric field lines must be continuous across the interface, such the electric field in the p-type side and the n-type side must equal each other at the interface or when x = 0. The maximum electric field occurs at the junction between the p- and n-type material. The integration constants C 1 and C 2 can be determined by using the depletion approximation, which states that the electric field must go to zero at the boundary of the depletion regions. The depletion region in the p- and n-type side respectively, measured from the physical junction between the two materials. Ε 0 is the permittivity in free space, and ε s is the permittivity in the semiconductor and -x p and x n are the edges of The only equation left to solve is Poisson’s Equation, with n(x) and p(x) =0, abrupt doping profile and ionized dopant atoms. All dopants are ionised ( N A += N A, N D + = N D).Abrupt or step doping profile ( N A +, N D + are constant in their respective regions).Similarly, J p is also constant across the depletion region. This means that J n is constant across the depletion region. No free carriers means (1) transport equations drop out and (2) no recombination or generation, so the continuity equation becomes We can assume no free carriers since the electric field sweeps them out of the depletion region quickly.No free carriers ( n(x), p(x) = 0 ) in depletion region.Depletion approximation: the electric field is confined to the junction region and there is no electric field in the quasi-neutral regions.Can solve for both the maximum electric field and the total depletion width.Īs stated on the previous page we need to make certain assumption to solve the diode equations analytically.Based on these assumptions, can use Poisson's Equation to develop a solution for the depletion region.Major assumptions: depletion approximation, no free carriers in this region, dopant concentration is constant. ![]() ![]() The Curse has green skin, although the part of his face around his eyes are red, and the eyes themselves glow a searing yellow. He has a golden helmet that has green shrubbery above it alongside his green rabbit ears, with the front having a realistic depiction of the eyes and snout of a lion. He is Springtrap's fourth animatronic skin, chronologically after Clown Springtrap, Flaming Springtrap, and Toxic Springtrap. The Curse is Springtrap's Aztec skin available on Mafor the Ancient Equinox Event. “ An Aztec-themed animatronic skin for the Springtrap plush suit in Special Delivery. Serpent Mangle carries miniature versions of both the sun and the moon, with the tiny sun giving off a small glow of light. The second head, as usual, has Serpent Mangle's right eye. Mangle's second head is inside the mouth of a fake dragon head. Their left eye is a regular one with a glowing yellow retina, and their right eye is entirely orange, similar to the sun. There is also a big bushy tail behind his back with the same orange and white color scheme. Their feet are mismatched in color, with their left foot being clothed in a green more organic looking foot, while the right foot is the same golden yellow as the rest of its body. Serpent Mangle has wooden brown teeth, golden brick on their cheeks and around their snout and a giant dahlia flower with orange and white petals around their neck. Their endoskeleton arms and legs are laced with red, green and yellow components. Serpent Mangle has green coloring on their head and hands. ![]() They are Mangle's second animatronic skin, after Magician Mangle in the Dark Circus Event. Serpent Mangle is Mangle's Aztec skin available on Mafor the Ancient Equinox Event. The sound commonly heard when Phantom Freddy is walking outside the Office window.“ An Aztec-themed animatronic skin for the Mangle plush suit in Special Delivery. This is shared with Springtrap and the rest of the phantom animatronics, aside from Phantom Mangle and Phantom Puppet. The sound Phantom Freddy makes when jumpscaring the player. Warning: The audio clips from the following list are loud! Audio He also appears to be damaged somewhat, with tears in his costume.Īppears on cardboard cutout from Curse of Dreadbear DLC. He now uses Classic Freddy's model from the original Five Nights at Freddy's albeit transparent in places, revealing the endoskeleton underneath. In Five Nights at Freddy's: Help Wanted, Phantom Freddy sports a completely different look. Upon closer inspection and brightening, he appears to be colored golden or at least green, though this may simply be from his burnt appearance or the overall green hue of the game, as the other phantom animatronics share the same properties of his color scheme. He also has an additional wire sticking out of his left eye socket as shown in Ultimate Custom Night, which Golden Freddy didn't have. His teeth appear to be slightly green (but this is likely down to lighting). His two lower legs are never seen in the game, but through his walking animation, the lower right leg looks ripped out and torn from his body. ![]() His mouth can usually be seen hanging open. He appears to be charred or burnt, possibly foreshadowing the fire that broke out in the establishment. Phantom Freddy has the same details as Golden Freddy from Five Nights at Freddy's 2, but instead has white pin-pricked pupils in his eyes like the other phantoms. He is a damaged and burnt hallucination of Freddy Fazbear from the second game. Phantom Freddy is one of the secondary antagonists and six phantom animatronics who first appeared in Five Nights at Freddy's 3. ![]() ![]() ![]() Our experimental results settle the seeming controversy between the classical and quantum properties of the Duffing oscillator and provide support to the recent results of the Liouvillian spectral theory 18, 19, 20, 21. Our experimental setup allows for a proper control of the initial state at different parameter settings as well as a high time resolution readout. Besides the wide tunability range of sample parameters in one device, the pulsed heterodyne measurement distinguishes our experiment from the experiments already reported in the literature. Here, we use an in-situ tunable superconducting nonlinear resonator to simulate the non-equilibrium quantum dynamics of the Duffing oscillator. These experiments are performed around a fixed parameter setting in a continuous-wave measurement setup. Recently, signatures of dissipative phase transition (DPT) have been observed in the scattering coefficient 14, 15, decay rate 15, 16, and second-order correlation function 17 of the Duffing oscillator, which indicate a prominent role of the quantum fluctuation in the SS. However, the seeming two classical SSs are still observed even in a typical quantum experiment setup 5, 6. These two perspectives indicate fundamentally different behaviors of the Duffing oscillator. However, it has been revealed by Drummond and Walls already in the 1980s that a fully-quantum treatment of the Duffing oscillator yields a single unique SS over the entire parameter space, such that it does not exhibit bistability or hysteresis 13. The underlying double-well potential model has been used to explain a variety of physical processes, such as optical bistability 7, 8, parametric amplification 9, 10, and self-oscillation 11, 12. This classical behavior of the Duffing oscillator has been observed in a considerable number of experiments, for example, in superconducting quantum circuits 4, 5, 6. Thermal fluctuations may induce unpredictable jumps between the two potential wells and lead to the bistability of the oscillation amplitude 3. Depending on whether the system is initially at rest or in strong oscillation, the oscillator spontaneously chooses one of the amplitudes when adiabatically tuning the parameters into the hysteretic regime. It gives rise to a hysteretic behavior where two different amplitudes of the forced oscillation are possible. In a certain parameter regime, classical mechanics predicts a double-well potential that allows two steady states (SSs) at the same parameter setting 2. The Duffing oscillator is a simple but prototypical model in nonlinear physics, which describes a forced oscillation with cubic (Kerr) nonlinearity and linear viscous damping 1. Our results reveal a smooth quantum state evolution behind a sudden dissipative phase transition and form an essential step towards understanding the intriguing phenomena in driven-dissipative systems. By engineering their lifetime, we observe a first-order dissipative phase transition and reveal the two distinct phases by quantum state tomography. They have a remarkably long lifetime but must eventually relax into the single unique steady state allowed by quantum mechanics. We demonstrate that the two classically regarded steady states are in fact quantum metastable states. Here, we measure the non-equilibrium dynamics of a superconducting Duffing oscillator and experimentally reconcile the classical and quantum descriptions as indicated by the Liouvillian spectral theory. However, this interpretation fails in the quantum-mechanical perspective which predicts a single unique steady state. The non-deterministic behavior of the Duffing oscillator is classically attributed to the coexistence of two steady states in a double-well potential. ![]() |
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