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On December 10th OPBF Super Featherweight champion Hironori Mishiro (8-0-1, 3) [三代大訓] will make his next defense, as he takes on 23 year old challenger Yoshimitsu Kimura (12-1, 7) [木村吉光]. Today we can confirm that that bout is set to be shown on TV, albeit on tape delay, as part of TBS's "Guts Fighting" series of shows.
For Mishiro the bout will be his 4th defense and promotional company Watanabe Gym seem to view his rise as something worthy of serious attention. They have already pushed him on to the fast track to the top, and he won the title in just his 6th professional bout, taking a decision over Carlo Magali. Although he failed to unify the title with the Japanese belt, fighting to a draw in 2018 with Masaru Sueyoshi, it's clear that his team have big plans for him, and likely see him as their successor to former WBA world champion Takashi Uchiyama. Since winning the belt not only has Mishiro retained it, with the draw, against Sueyoshi but also scored notable wins over Takuya Watanabe and Ryo Takenaka.
As for Kimura this will be a second shot a belt for him, following a competitive loss to Richard Pumicpic for the WBO Asia Pacific Featherweight title. Since that loss Kimura has moved up in weight and has built some momentum coming in to this bout.
The bout will be aired aired just days later, with the broadcast also expected to help promote the New Year's Eve card which TBS will be showing live.
At the moment it's unclear whether TBS will also air some form of footage of the very interesting chief support bout between Yudai Shigeoka (1-0, 1) [重岡優大] and OPBF Minimumweight champion Lito Dante (16-10-4, 8).
(Image - TBS)
Yudai Shigeoka to face OPBF champion?
According to one, often reliable, Japanese source Japanese prospect Yudai Shigeoka (1-0, 1) [重岡優大] is set to return to the ring on December 10th in a 6 round bout against a current OPBF champion, albeit in a non-title bout.
The source has revealed that Shigeoka is pencilled in to face OPBF Minimumweight champion Lito Dante (16-10-4, 8), who fights for the first time since scoring a huge upset win in March against Tsubasa Koura.
The talented Shigeoka, the older brother of WBO Asia Pacific champion Ginjiro Shigeoka, debuted at the end of October and looked sensational as he beat Thai foe Manop Audomphanawari. This is, however, a massive step up in class and shows the youngster's ambition to rise through the ranks in an incredibly aggressive way.
Dante on the other hand is pretty a card carrying member of the "who needs him? club". The Filipino might be the OPBF champion but even with that belt he is high risk and low reward, and over 12 rounds he's a nightmare due to his toughness and energy. He can be out-boxed over the shorter distance, as Shigeoka appears to be planning here, but he is still not an easy out for any one.
The bout is said to be pencilled in as the chief support bout for a Dangan card headlined by Shigeoka's stablemate Hironori Mishiro (8-0-1, 3) [三代大訓] defending the OPBF Super Featherweight title against 23 year old challenger Yoshimitsu Kimura (12-1, 7) [木村吉光].
Other fighters now pencilled in for this card include Fumiya Fuse (8-1, 1) [富施郁哉] and Ayaka Miyao (23-8-1, 6) [宮尾 綾香], though neither of these two have had opponents reported by our source yet.
Given the sheer number of announcements and big fights over the last few days it was obvious we were going to miss something, and sadly one of the stories we missed was actually quite and interesting one, as Hironori Mishiro (8-0-1, 3) [三代大訓] has his next OPBF Super Featherweight title defense announced.
The unbeaten fighter from the Watanabe Gym will be back in the ring at Dangan 231 on December 10th at the Korakuen Hall, where he will face 23 year old challenger Yoshimitsu Kimura (12-1, 7) [木村吉光], who is having his second title bout, following a loss in a WBO Asia Pacific Featherweight title bout against Richard Pumicpic.
The talented Mishiro will be looking to make his 4th defense of the OPBF title, and build on wins from earlier this year against Takuya Watanabe and Ryo Takenaka. Since turning professional he has been on the fact track, winning the OPBF title in 6th bout, when he beat Carlo Magali, and was unlucky not to unify the belt a fight later, when he fight to a draw with Masaru Sueyoshi. Sadly though this will be his 4th defense against a Japanese opponent, and it feels as though maybe fighters from across the Orient don't have the same desire for the belt that they once had.
Whilst Kimura lost against Pumicpic he has been touted highly and won the 2016 Rookie of the Year, beating Tsuyoshoi Sawai in the Featherweight final. Since losing to Pumicpic we've seen him move up in weight and score 3 straight stoppage wins, whilst looking like a heavier handed fighter at 130lbs than he was at 126lbs. Despite that success at Super Featherweight he will be seen as the under-dog in this bout.
At the moment no other bouts have been confirmed for this card, though with is likely being the final big Dangan card of 2019 we are anticipating at least 1 other very notable bout to be added to the show in the coming days.
Earlier today at the Korakuen Hall the East Japanese Boxing Assocation award winners for the month of July were given a chance to collect awards and speak to the crowd, who were there primarily to see the East Japan Rookie of the Year semi-finals.
The MVP for the month was OPBF Super Featherweight champion Hironori Mishiro (8-0-1, 3) [三代大訓], who retained his title with a win over the now retired Ryo Takenaka (18-5-1, 11) [竹中 良]. Mishiro retained his title by stopping Takenaka in the 8th round of their clash.
At today's ceremony Mishiro said he was pleased to have won the MVP award following successive fights and that his next bout would be in December, with more details being revealed over social media in the near future.
The Fighting Spirit award was won by Japanese Bantamweight champion Yusuke Suzuki (11-3, 7) [鈴木悠介] following his violent war with the heavy handed Yuta Saito (12-10-3, 9) [齊藤裕太]. Thankfully Saito's face, which was a mess after the bout, has healed up well. He didn't say much but did say that next time out he'll be doing his best to win the MVP award.
For those who missed the Suzuki Vs Saito bout we've included it below.
The Newcomer award won by the fact rising Light Welterweight hopeful Andy Hiraoka (14-0, 9) [平岡アンディ], who took a decision win over former world title challenger Akihiro Kondo (31-9-1, 18) [近藤 明広]. Hiraoka mentioned going overseas in the future and that he was honoured to recieve his first award. At the moment there is no future plans set in stone, but he will be announcing things in the near future through social media.
(Image courtesy of boxmob.jp)
Earlier today we saw an announcement from Japan revealing that wformer OPBF Featherweight champion Ryo Takenaka (18-5-1, 11) [竹中 良] was retiring following his recent loss to OPBF Super Featherweight champion Hironori Mishiro (8-0-1, 3) [三代大訓].
The talented Takenaka was an amateur standout, running up a 73-17 (28) record in the unpaid ranks before beginning his professional career in 2008.
Despite some set backs early in his career, including losses to Ryol Li Lee and Hisashi Amagasa, Takenaka would win the OPBF Featherweight title in 2015, with a brilliant KO over Vinvin Rufino.
As the OPBF champion Takenaka made 3 defenses before being stopped by Korean tough guy Sa Myung Noh in 2017. A move up in weight followed and after two wins he would be upset by the unheralded Heorhii Lashko before losing in his final bout to Mishiro.
News! We try and give you the most interesting news stories from the Asian boxing world!
December 2019


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Size of stripe domains in a superconducting ferromagnet
In a superconducting ferromagnet, the superconducting state appears in the ferromagnetic phase where usually a domain structure has already developed. We study the influence of the superconducting screening currents on a stripe structure with out-of-plane magnetization, in a film of arbitrary thickness. We find that superconductivity always induces a shrinkage of the domains, and there is a critical value of penetration depth below which a mono-domain structure is more stable than the periodic one. Furthermore we investigate the possible different effects of singlet and triplet superconductivity on the domain width, as well as the conditions for the existence of vortices in the domains. The obtained results are then discussed in light of the experimental data of superconducting ferromagnets URhGe, UGe2, and UCoGe.
pacs:75.60.Ch, 74.20.De, 74.25.Ha, 74.70.Tx
I Introduction and model
In the discovered Uranium-based superconducting ferromagnets (SFM) UGe saxena (), URhGe aoki2001 () and UCoGe huy () the Curie temperature is much higher than the superconducting critical temperature which means that superconductivity appears in the ferromagnetic state where it is usually a domain structure (DS) which develops. In previous works krey (); bulaevskii (); sonin1 (); faure (); sonin2 () the influence of the superconducting screening currents on the DS has been studied in the case of thick or bulk systems, when the thickness along the easy magnetization direction is much larger than both the transverse domain width (see Fig. 1) and the London penetration depth . The domain period at equilibrium results from the balance between a positive contribution to the energy density due to domain walls and a negative contribution from the magnetic induction, as the magnitude of both increases when is reduced. An exact energy minimization faure () shows that for the condition (where is an effective domain wall width that parametrizes the wall energy) superconductivity decreases the domain size due to partial penetration of the magnetic field near the domain wall. This energy decrease is proportional to and the formation of the domain wall is favorable when this contribution counterbalances the energy of the domain wall itself, which is proportional to . For the system is in a mono-domain state without any domain wall faure (); sonin1 (); sonin2 (). In the present article we extend Fauré and Buzdin's work faure () by deriving the expression of the energy valid for any thickness and we discuss the DS in all limits, in particular when . Furthermore we investigate the possible effects of singlet and triplet superconductivity on the DS, as well as the conditions for the existence of vortices in the domains.
Model.— We consider a ferromagnetic film of thickness that can also become superconducting (see Fig. 1). The -axis is chosen perpendicular to the film with the surface edges at . Domain walls parallel to the -plane separate the periodic ferromagnetic structure into domains of equal width and with magnetization alternating along the -axis, i.e. with
This means that we consider the domain wall thickness very small compared to and . The energy per surface unit is where the magnetic field energy is given by the relation
and the superconducting current energy is expressed in the London limit degennes () (i.e. the superconducting coherence length )
Here, is the total area the film surface. The explicit dependences with respect to the domain width result from the Ansatz we made for the magnetization . The contribution from the domain walls may be written as faure ()
where is a domain wall characteristical length scale. Usually provides an upper limit of the real domain wall width faure (). Hereafter, the temperature will be considered phenomenologically within an explicit dependence of the London penetration depth . The latter is finite in the superconducting low phase, and diverges at the critical temperature .
Outline of the article.— In the second section we analytically calculate the field distribution and the energy of a periodic stripe DS in a SFM of arbitrary thickness. An exact expression of the energy is obtained as an infinite sum. In section III the equilibrium size of the domains is determined in the superconducting state as a function of the penetration depth. Analytical expressions of the domain width are obtained in limit cases. The stability of the domain structure is also discussed. We then investigate the difference between singlet and triplet superconducting states. Specifically, the triplet pairing is described by a domain wall energy which is temperature dependent, in contrast with the singlet pairing. In section IV we draw the condition for vortices appearance at the center of a domain. Finally in section V we apply our results to the DS in Uranium-based superconducting ferromagnets before concluding.
Ii Method of solution
First, we minimize the energy with respect to the magnetic induction . This yields the London equation in the film and outside. Once is found by solving the London equation, the resulting total energy, , will be minimized with respect to to determine the domain width at equilibrium.
ii.1 Magnetic field
We find the magnetic induction by Fourier expansion. Using Maxwell-Thomson equation and symmetry relations and , the field can be written as
where we remind that . When solving the London equation in the film and Maxwell's equation outside, we use the symmetry condition and the continuity condition at the surfaces. This yields, for ,
and for ,
Figures 2 and 3 show the distribution of the magnetic field in the normal state and the superconducting state. It is plotted between the domain wall and the domain center. In the normal state, the magnetic field distribution in a wide domain () is concentrated around the domain wall (see Fig. 2(a)) while in a narrow domain () it is nearly uniform and equal to (see Fig. 3(a)). The supercurrent screens the field around the domain wall on a length scale (compare for example the contour in (a) and (b) of Fig. 3). Note that the supercurrent is responsible for a kink that the lines of constant show at the film surface (see Fig. 2(b) and Fig. 3(b)). This is because is discontinuous at the interface when . Flux lines also have a kink at the domain wall since the magnetization is discontinuous there.
ii.2 Energy of the domain structure
To simplify the expressions of the energy it is convenient to introduce the normalized lengths
where is Pearl's penetration depth which, in the limit , takes the place of as the effective magnetic length scalepearl (). Note that in these notations . Furthermore we will consider the normalized energy and omit the bar henceforth. So the domain wall contribution is and the volume contribution, is
where and . For a thick film, i.e. so that , Fauré and Buzdin's result faure () is recovered as expected. Since the limit has been previously investigated faure () we discuss below the limit , that is , with more details.
ii.2.1 Regime
This parameter regime is realized in the normal phase where , as well as inside the superconducting phase, in the vicinity of the critical temperature . When (i.e., when ), the sum in (10) may be expanded in powers of before summing. Hence for ,
while for ,
ii.2.2 Regime and
This parameter regime may be realized in the superconducting phase, for either thin films or large domains. When the sum in (10) can be approximated by an integral. Euler-MacLaurin's approximation yields
where the is defined by Eq. (42) in the Appendix. Then using asymptotic expression (43) of in the limit , one finds
and for , asymptotic expression (44) yields
Iii Domain width at equilibrium
iii.1 General results
The equilibrium size is obtained by minimization of the total energy . Figures 4-6 show as a function of the penetration depth for different values of the normalized wall thickness . In the superconducting state decreases with decreasing temperature from infinity at to a finite value at . As discussed below, just below the domain width always decreases from the normal state value realized for . One can distinguish two regimes. When the domains in the normal state are wide () the decrease is negligible, while when the domains are narrow () their width can drastically shrink down to . Then, in both regimes, reaches a minimum value before diverging at a critical lower bound . This limit corresponds to the situation where the ferromagnetic induction is completely screened by the supercurrent faure (); sonin1 (); sonin2 () and there is no stray field that need to be accommodated by a DS.
The -dependence of the width is similar to the prediction for DS in superconductor-ferromagnet (S/F) bilayers bilayer (); stankiewicz () except for two aspects. First the shrinkage factor in a S/F hybrid is limited and bilayer (). Experiments performed on heterostructures made of a ferromagnetic garnet layer combined with a superconducting layer of Pb tamegai () or Nb vlasko-vlasov () have observed the shrinkage of the domain size due to superconductivity. The smallest observed shrinkage factor was substantially smaller than the theoretical prediction . This circumstance is a non-equilibrium effect and is related to the special dynamics of the vortex structure created in the superconducting layer and coupled to ferromagnetic domains vlasko-vlasov (). The second point is that although the DS can also be unstable in S/F bilayers when decreases, it exists a range of parameters (when the thickness of the F-layer is approximately larger than half the domain width in the normal state) in which remains finite even in the limit stankiewicz (), in contrast with SFM where the DS is never stable for a vanishing .
Hereafter, complementary to the exact numerical solution, we present the analytical results obtained in various asymptotic regimes.
iii.1.1 Normal state and vicinity of the transition
In the limit , using expression (11) valid for the vicinity of the superconducting transition where , one finds that the minimum of the energy is realized at
which yields the domain width
in the normal state (see Fig. 7). The domain width just below the superconducting transition is then related to the normal-state width by
iii.1.2 Stability of the periodic domain structure
The periodic domain structure is always stable in the normal state where the energy minimum is obtained for a finite width . This is not the case in the superconducting state. In the limit and , the saddle-point equation for the energy is
where the function is defined by Eq. (42) in Appendix. There is an energy minimum at a finite only for . Since increases with , this condition defines a lower bound below which the periodic structure is unstable. In the thought experiment where decreases from infinity (normal state) to zero, the period first decreases from but then it increases back before diverging as (see Fig. 4). Note that the limit of vanishingly small has been considered in Ref. sonin1 () and the conclusion of the absence of DS was made. When in the normal state, the approximations of yield
while when the normal-state width , the periodic structure exists down to
Figures 8 and 9 show that these analytical relations fit well the numerical results in the limit regimes.
One can now understand the difference of shrinkage factor between a narrow domain and a wide domain. For a narrow domain with and , the width in the superconducting state decreases with the penetration depth as . The shrinkage goes on until the DS is destabilized by an excessive superconducting screening. The minimum value that the width can have is then , which is much smaller than . In the opposite limit when and , the actual magnetic length scale is , not . And the domain width behaves as when is smaller than . Thus the minimum , so that a wide domain does not significantly shrink while the penetration depth decreases to the instability value .
iii.2 The case of triplet superconductivity
As we will see in a next section, the temperature dependence of the domain equilibrium size can provide a phenomenological way of distinguishing triplet from singlet pairing. Here, we describe the general formalism; numerical applications to some specific compounds will be shown later as examples, in the framework of Uranium-based superconductors.
iii.2.1 Modification of the wall energy due to the depletion of condensation energy
In the case of a triplet superconductor with Cooper pairs fully spin polarized by the intrinsic magnetization of the ferromagnetic domains, a depletion of the order parameter occurs on a width at both sides of the interface separating two domains of opposite magnetizations. This inhomogeneity results in a loss of condensation energy at a domain wall. At a first approximation the domain wall energy for is modified by replacing the effective domain wall width by the temperature dependent defined by
where , and
is proportional to the ratio of the superconducting energy at to the magnetization energy. Here, we have assumed , , and . Using the asymptotic expressions relating to the normal state width , one can estimate from experimental data in the limit with
and in the limit with
iii.2.2 Behavior of the domain width below the transition
A triplet order parameter yields a vanishing correction to the domain wall energy at the transition. The temperature dependence of the domain size is in the limit ,
and in the limit ,
So, as in the singlet case, always decreases with decreasing temperature in the vicinity of . However at a lower temperature and for a large parameter , the behavior for the triplet case can be significantly different from the singlet case. Since for a given there is an universal curve for the singlet pairing, it is possible to detect an experimental signature of triplet superconductivity as a deviation from this curve. This is schematically illustrated in Fig. 10 which shows the temperature dependence of in the singlet and in the triplet case. When temperature is reduced from (on the right side where ) to (on the left side where ), the -curve in the triplet case interpolates between the curve (a) obtained with a constant and the curve (b) for . The triplet-case curve follows the singlet-case curve with at high temperature but at a lower temperature a deviation appears which is maximum at .
In the expression (29) of for the triplet pairing, the first-order term is proportional to while the second-order term is proportional to so one can expect that the singlet/triplet discrepancy can be amplified when reducing the thickness of the film. As shown in Fig. 10 this discrepancy is enhanced when the ratios and become larger. For small enough thickness the difference is not only quantitative but is also qualitative as the triplet-pairing curve can increase with decreasing temperature while the singlet-pairing curve decreases.
Iv Condition for vortex appearance
In this section we estimate the energy for the creation of a vortex-antivortex pair in the middle of adjacent domains. This additional energy is the sum of (i) the energy decrease when (anti)vortices are driven by screening currents away from domain boundaries to domain centers and (ii) the concomitant increase of the interaction energy between one vortex and its antivortex as they move apart from each other. For simplicity we neglect the vortex-core energy assuming the limit of large .
iv.1 Energy decrease due to the screening current
The force of the screening current acting on a vortex degennes () is , where the quantum of flux T.m. When the vortex moves from the domain wall to the domain center, the current then produces a work equal to
where is the coupling energy of the flux carried by one vortex with the magnetization of a ferromagnetic domain.
The work has simple analytical expressions in limit cases. In the regime ,
where the Lerch transcendent . If furthermore , expression (31) can be simplified as
Thus increases with the width of the domain and, when the latter becomes large compared to the magnetic radius of a vortex, the work is simply equal to the coupling energy .
In the opposite regime , the screening current is vanishingly small so its work is only equal to a fraction of . For wide domains (), the dependence of on the domain width is linear as
where Catalan's constant , while for narrow domains (), the dependence is quadratic as
iv.2 Interaction energy of a vortex-antivortex chain
The interaction energy of a chain composed by one vortex (antivortex) located at the center of every domain of positive (negative) magnetization is the magnetic energy required to separate by a distance vortices and their paired antivortices created at domain walls. In the case or , the energy per one vortex buzdin () has the asymptotic expression
We have assumed . In a large- superconductor with , there is always a temperature regime close to in which .
In the opposite limit, for the interaction energy per vortex is
while for , it is
iv.3 Condition for the appearance
From the above results we can derive the condition of the vortex stability in a superconducting domain structure. The latter is assured when the total energy per vortex is negative. This condition defines a critical value of magnetization above which vortices appear. One can distinguish four regimes in which has a simple analytical expression. In a film with narrow domains (i.e. ),
Note that Eq. (38) recovers the expected result that vortices appear when the magnetization exceeds the lower critical field of a non-magnetic superconductor defined as . However, when the penetration depth is larger than the domain width, the coupling of the vortex flux with the DS magnetization is not energetically optimum so the critical magnetization (39) is higher than the mono-domain value .
V Application to Uranium-based superconducting ferromagnets
According to experimental data (see Table 1), the Uranium-based superconductors UGe, UCoGe and URhGe are in the limit . The effective domain wall thickness can then be easily calculated in this limit from the experimental value of the domain width in the normal state. We roughly estimate the zero-temperature condensation energy with the BCS formula where is the volumic specific heat jump at . Among the three compounds UCoGe has the smallest magnetization resulting into the largest (see Table 1). It is then the most promising candidate where to look for possible observation of the non-monotonic temperature dependence of the domain width in the superconducting phase. Using its estimated parameters we plotted the temperature dependence of the domain width for the singlet and the triplet scenario in a film of half-thickness mm (Fig. 11) and m (Fig. 12). For mm (Fig. 11) the domain width decreases below in both the singlet and the triplet case but there is a significant difference of size at between the two. By reducing the film thickness the discrepancy is amplified. For instance with m (Fig. 12) one obtains a qualitative difference: for the triplet case the width increases by 32% from its value in the normal state while for the singlet case it shrinks by 21%.
Vi Conclusion
We have done the complete analysis, within the London approximation, of the domain width at equilibrium in a SFM film of arbitrary thickness . We have shown that the ratio follows a universal dependence on the normalized penetration depth and the normalized effective wall thickness (see Figs. 4-6). In addition to the exact numerical dependence, we have derived analytical expressions of this relation in limit cases. In particular, we have recovered the previously published results by Fauré and Buzdin faure () which had been established for and , and we have complemented them with the analysis in the opposite limit and .
We have found that the domain width always decreases with temperature when the DS enters the superconducting phase. The screening supercurrent induces a decrease of the domain width if the latter is larger than the penetration depth. However, the paramagnetic screening suppresses the DS below a critical value of penetration depth, which means that the system may become mono-domain at a finite temperature if . The domain shrinkage is relatively small when the domain width in the normal state is much larger than the film thickness. Indeed, in this limit, the width decreases as which is only a fraction smaller than since . With the other limit shape of domains, i.e. , the shrinkage can be important since then the domain width decreases as while the critical penetration depth .
Furthermore, we have investigated the effect of the triplet pairing within an effective temperature-dependent renormalization of the domain wall energy. Actually, the DS magnetization alternatively suppresses the order-parameter components with opposite spin-projections. This inhomogeneity results in an additional positive contribution to the domain wall energy, that is absent for the singlet pairing. The supplementary term vanishes at the transition temperature but can be significant at a lower temperature. The variation of the domain width is then no more described by the universal dependence of on obtained for the singlet case. This gives a phenomenological way of distinguishing triplet from singlet pairing in experiments. And, as we have shown, the discrepancy can be amplified by reducing the film thickness (see Figs. 11 and 12).
We have also established that vortices can appear when the magnetization exceeds a critical value . In narrow domains (i.e. ), the latter is equal to the lower critical field of a non-magnetic superconductor if , but in the opposite limit , it is much larger than . For wide domains (i.e. ), we have found that the critical magnetization behaves similarly, with the difference that is then replaced by Pearl's effective penetration depth .
The available experimental data (Table 1 and Ref. saxena (); ureview (); uge2 (); sakarya (); huy (); ureview (); ucoge (); hykel (); aoki2001 (); ureview (); urhge (); dolocan ()) for UGe, URhGe and UCoGe show that in these compounds and the conditions for the vortices appearance (section IV) are fulfilled. This means that the effects of domain shrinkage (considered in section III for the case where the vortices are absent) should be weakened. Another difficulty to experimentally observe the evolution in the superconducting state may be related with the pinning of the domain wall and/or vortex pinning. At present there are no convincing experimental data on the change of the domain structure below .
It has been recently observed in S/F bilayers tamegai (); vlasko-vlasov () that the coupling between vortices and magnetic domains leads to a strong shrinkage of domains in the presence of the oscillating field used for equilibration of the domain structure. It would be interesting to perform the similar experiments with superconducting ferromagnets to study these coupling effects.
We thank K. Hasselbach, C. Paulsen, J.-P. Brison, and D. Aoki for helpful discussions. This work has been supported by the French ANR project SINUS.
Appendix A The function
We define the function as the integral
a.1 Limit
The integral can be rewritten as
so by using the approximations in the numerator and in the denominator when , and when ,
Then for
a.2 Limit
In the limit , then
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- (21) N. T. Huy, D. E. de Nijs, Y. K. Huang, and A. de Visser, Phys. Rev. Lett. 100, 077002 (2008); P. de la Mora and O Navarro, J. Phys.:Condens. Matter 20, 285221 (2008); A. Gasparini, Y. K. Huang, J. Hartbaum, H. v.Lohneysen, and A. de Visser, Phys. Rev. B82, 052502 (2010); A. Gasparini, Y. K. Huang, N. T. Huy, J. C. P. Klaasse, T. Naka, E. Slooten, and A. de Visser, J. Low Temp. Phys. 161, 134 (2010).
- (22) D. Hykel, Microscopie à micro-SQUID: étude de la coexistence de la supraconductivité et du ferromagnétisme dans le composé UCoGe, PhD Thesis, University of Grenoble (2011).
- (23) K. Prokes, T. Tahara, Y. Echizen, T. Takabatake, T. Fujita, I. H. Hagmusa, J. C. P. Klaasse, E. Brück, F. R. de Boer, M. Divis, and V. Sechovsky, Physica B 311, 220 (2002).
- (24) V. O. Dolocan, Imagerie magnétique des supraconducteurs non conventionnels, PhD Thesis, University of Grenoble (2005).

subset: commoncrawl


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A new wife doesn't know anything admin | October 26, 2018 | Funny | No Comments A new wife doesn't know anything Related Posts A man lost his wife No Comments | Mar 3, 2019 Tea party No Comments | Sep 22, 2018 Student ask teacher about punishment No Comments | Apr 12, 2016 Late appointment with doctor No Comments | Feb 21, 2019 About The Author admin Add a Comment Cancel reply Your email address will not be published. Required fields are marked * Name:* Email Address:* Website: Save my name, email, and website in this browser for the next time I comment. Comment:* You may use these HTML tags and attributes:   <acronym title="">
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text: In towns across Somerset County, including Franklin Township, we have invested heavily in open space, and park preservation and improvements. The amenities at Franklin's Colonial Park include paddle boats, golf putting facilities, a tennis center, a leash free dog area, a new splash park and more. Take advantage and enjoy all that our Somerset parks have to offer.


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A Kenner man who crept into the bedroom of a friend's teen-age daughter pleaded guilty Tuesday to trying to sexually assault the 16-year-old, who managed to fight him off, authorities said.
Adrian Jauregui, 37, pleaded guilty to attempted first-degree rape, according to Jefferson Parish court records.
Judge Lee Faulkner of 24th Judicial District Court sentenced Jauregui to 10 years in prison. Faulkner also ordered Jauregui to register as a sex offender for the rest of his life once released.
The case was investigated by the Gretna Police Department. Jauregui was a friend of the girl's father and visited the family's Gretna home on March 9, Capt. Russell Lloyd, a department spokesman, said.
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Health Walks
Our regular Health Walks are a great way to see the beautiful landscapes of Winchester and take in some fresh air at the same time! Explained as 'a purposeful, brisk walk undertaken on a regular basis' these health walks can provide a great starting basis to leading an active and healthy lifestyle in a fun, friendly and relaxed environment.
Walk schedules
We currently have 9 walks within the Winchester district that are run by our team of Volunteer Walk Leaders. These weekly walks last for about an hour and are free of charge.
Day Time Where Details Monday 10.30am Opposite Antiques Market, Kings Walk, SO23 8AF The walk is split in to 3 walks
- Fast walk (3 miles approx)
- Steady walk (2 miles approx)
- Short walk (10-30 minutes)
Tuesday 10:30am The Square, Bishops Waltham (SO32 1GG) 30 minute pavement and path walk Tuesday 10.45am Coach & Horses Pub, Sutton Scotney, Oxford Road (SO21 3JH) One hour walk Tuesday 1.30pm Opposite the entrance to Alresford Recreation Centre, Alresford (SO24 9EP) One hour walk Wednesday 9.30am Kings Walk opposite Antiques Market, Kings Walk, SO23 8AF One hour walk Wednesday 10.30am Colden Common Community Centre, Colden Common (SO21 1UU)
One hour walk covering 2-3 miles
Thursday 10.30am The Square, Bishops Waltham (SO32 1GG)
- 1st Thursday of the month: non-stile walk.
- Last Thursday of the month: bus/car walk
Thursday 9:45am River Park Leisure Centre (SO23 7DD) 45 minute buggy walk Friday 10.00am Costa Coffee, Weeke Gate, Stockbridge Road, Winchester (SO22 6EL) One hour walk covering 2-3 miles 'bus walks' The group catch a bus to another location and either walk back from there or they do a circular walk in that area, then catch the bus back. 'car walk' When a location is not accessible by bus, the group gets there by sharing cars; they then do a circular walk in that area, then drive back.
How to take part
If you'd like to take part, all you have to do is come along to the start point of one of our walks a few minutes early, so that one of our trained walk leaders can give you a registration form (see link on this page in Documents) to complete. Then you're free to take part in as many walks as you like, as often as you like. If you want to know more before you start, just get in touch on firstname.lastname@example.com or call 01962 848 493 / 07920 417183.
Please complete this registration form on the link below to fill in your registration online: https://www.walkingforhealth.org.uk/login
These walks rely on the support that we receive from our local Volunteer Walk Leaders and we are always looking for more volunteers to join our team. Walk Leaders attend a one day course to become qualified, the course is free of charge and run in the local area. Once qualified a leader can choose to take a group walk on a regular basis or on a more infrequent basis as they wish.
Become a Walk Leader
We are always looking for enthusiatic volunteers to become one of our walk leaders, ff you are interested please contact us on email@example.com or 01962 848 493


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DescriptionBrowning Citori Model Over & Under Shotgun.
Serial no. 13737N57, 20-gauge [2 3/4-inch], 28-inch barrels with ventilated rib and white dot bead sights. Blued finish. Gold-plated trigger. Checkered walnut pistolgrip stock and fore-end. Ventilated factory rubber recoil pad. Made in Japan. Length of pull: 14 1/2-inches. Weight: 7-pounds, 12-ounces. From The Estate of Ronald Martin.
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What does it take for a television series to be successful? Perhaps it has something to do with a good script or really good actors. Maybe it's an interesting story and maybe it is just because the right demographic of viewers are watching the show.
Recently an American television network cancelled their shows based purely on the fact that these shows were not attracting the 'younger audience'. These shows were extremely popular amongst the older demographic but this didn't seem to matter because the younger audience in where the money is.
According to an article in the Wall Street Journal, this is mainly due to 'the obsession of advertisers with younger viewers'. The article goes on to say,
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It's true, to an extent, we don't really think about the elderly when we advertise, we often hear the words, 'young, hip and fashionable' when it comes to selling a product. Of course there are many arguments to this, and let's all be honest, like all major industries in existence, it is mainly about making money.
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Who would have thought that one day you will be too old to watch television?


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Features :
Model Number 1812868
Maximum Weight Recommendation 18 Kilograms
Care Instructions Wash removable seat cushion in cold water on delicate cycle and line dry. To clean stroller frame, use only household soap and warm water. Never use bleach. If wheels squeak, use a light oi.
Batteries required No
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Number of reclining positions 1
Item Weight 18 Kg
Product Dimensions 58.4 × 72.4 × 102.9 cm
Item model number 1812868
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Bradberry Metal 24 Bar Stool (Set Of 2) New Design
When you need greater than a Bradberry Metal 24 Bar Stool (Set Of 2), you convert to sleeper couches. They're good as they're multi-functional. Plus they are irreplaceable in tiny spaces. You can have visually appealing seating to support guests, and at precisely the specific same time, they could dual as beds when you have sleepovers. Here is our top 10 list of the best Bradberry Metal 24 Bar Stool (Set Of 2) or Bar Stools 2. When researching them, we made sure that they weren't simply well built, sturdy and easy to use but attractive in their layout also. Bringing among them home you won't harm your decoration, and you could decide on the style to match. We have upgraded this list for 2019, to help you make certain you're picking from the latest choices.
This modern and minimalist set of bar stools would be a perfect addition to your living space. The metal framework provides durability and sturdiness to these bar stools. The woven fabric upholstered seat provides the utmost comfort. The contrast of the gray seat and the black base is quite appealing. The angular base has footrest for keeping your feet comfortable while seating on the stool. The bar stools can be used as additional seating or paired up with counter tables. Also, the stools has...Seat Material: UpholsteredFrame Material: MetalUpholstery Material: Linen BlendBase Color: GraySeat Color: Gray
Top 10 Bradberry Metal 24 Bar Stool (Set Of 2)
1 Adjustable Height Swivel Bar Stool Wildon Home®
If you want a stronger solid base, depending on the type of flooring you choose, add a layer of hardcore to a depth of roughly 5cm to 8cm over the area of the patio.
It looked to me at first as if something that would be better thrown out than used or at the very least painted but I have done so much of it now at the request of my customers that the look has actually grown on me and I have several pieces of it in my home.
Enjoy your morning coffee or an evening cocktail on this island-inspired counter stool, featuring a woven design.Seat Material: WickerRattanFrame Material: WoodWeight Capacity: 200lb.Base Color: NaturalSeat Color: Natural; whitewash
2 Entin Wooden Bar Stool (Set of 2) Red Barrel Studio
There are a few different types of fabric used on patio furniture, including acrylic-based fabric, olefin, polyester and PVC-coated polyester or vinyl, and mold can be removed from these fabrics fairly easily.
Apart from other kinds of furniture, Tomas Chippendale was also a trendsetter in terms of chairs, and more particularly dining room chairs, and the Chippendale style of chair became highly popular.
This Chevy Racing 31inch Swivel Bar Stool will provide you and your guests with a comfortable seat as well as a stylish accent to your game room, garage or collection. The stool's seat features an authentic logo highlighted by resilient marine grade vinyl sides and top trimmed with quarter inch vinyl beading. The seat also includes luxurious foam padding and a 360 degree swivel. The seat back provides added support and extra comfort. Chrome double rung reinforced legs are made of tubular steel...Seat Material: Plastic/AcrylicFrame Material: MetalWeight Capacity: 300lb.Base Color: ChromeSeat Color: Black
3 Adjustable Height Swivel Bar Stool Bare Decor
Be sure you have enough space to comfortably house the furniture.
Pressure treated wood is wood that has undergone several treatments with chemical preservatives under high pressure so that the chemicals seep deep into the wood and serve the wood to become more durable and pliable to termites, fungus, rots and water.
With its low back and neutral hues, this 30.75inch bar stool is brimming with understated appeal. Crafted from metal in a versatile black finish, its frame features four tapered legs connected by a convenient footrest to support up to 300 lbs. Foam fill provides a bit of cushioning as you take a seat, while polyester fabric upholstery in a light gray tone envelops the square seat, back, and arms for an approachable look. The manufacturer backs this product with a 10-year warranty. Assembly is...Seat Material: UpholsteredFrame Material: MetalUpholstery Material: 100% PolyesterWeight Capacity: 300lb.Base Color: Textured Black
4 Fontenay Bar Stool One Allium Way
Sometimes touch up paint is included with the purchase of wrought iron patio furniture.
Large pillows covered with rich woven wool pillow covers placed around the room for comfortable floor lounging is a nice addition.
Seat Material: UpholsteredFrame Material: Solid WoodUpholstery Material: Polyester BlendWeight Capacity: 250lb.Base Color: Black
5 Afteroom 29 Bar Stool Menu
Wood is special and I love seeing them in children's toys.
But metal outdoor furniture has come a long way.
Seat Material: UpholsteredFrame Material: MetalUpholstery Material: Faux leather; VinylWeight Capacity: 255lb.Base Color: Chrome
6 Bolick 29 Bar Stool (Set of 2) Foundry Select
They can also be leather finish chairs in the Parson style of furniture.
However, you need to take into consideration that cast aluminum is nonporous, which means that paint will not adhere to the surface.
The clean lines of the bar stool complement any home from traditional to contemporary. With a birch wood frame in an espresso finish, is covered in antique brown PU leather with silver nail heads detailing its seat and gently curved back.Seat Material: Faux leatherFrame Material: Solid WoodUpholstery Material: Faux leatherWeight Capacity: 275lb.Base Color: Espresso
7 Moonsu Traditional 24 Swivel Bar Stool Bayou Breeze
Have you ever wondered what is so special about teak wood that it is in high demand globally?
Patio bar furniture can be purchased in water proof material so as to not leave dry guests soaking wet.
Perfect for pulling up to a pub table in the entertaining ensemble or when stationed around the kitchen island, barstools are always a stylish seat. Take this one for example: Crafted from manufactured wood, this piece boasts a contemporary design with a footrest and full swivel feature for your convenience. Upholstered in foam-filled faux leather, the adjustable seat lends an inviting feel to your ensemble and can support up to 250 lbs. after assembly.Frame Material: Metal; Manufactured WoodUpholstery Material: Faux leatherWeight Capacity: 250lb.Base Color: ChromeAssembly Required: Yes
8 Traditional Cedar Log 24 Bar Stool Fireside Lodge
Like the rest of Mallin's offering this range is very comprehensive and contains all the furniture pieces that you could possibly want, including rockers, loungers and beach chairs.
Giving a fresh coat of paint to your outdoor wooden furniture does not require the services of a professional.
Seat Material: UpholsteredFrame Material: Solid WoodUpholstery Material: Faux leatherWeight Capacity: 250lb.Assembly Required: Yes
9 Dekalb 27.75 Bar Stool Willa Arlo Interiors
If table was painted any time from the early to mid-20th century, you should double check for lead paint before sanding.
Good drainage is achieved by sloping the patio floor away from the house and make sure that the slope is effective enough to stop rainwater from backing-up to the house through the door's floor gap.
Made for the ultimate sports fan, impress your buddies with this knockout from Holland Bar Stool. This contemporary logo stool has a single-ring base and a cushioned back to achieve maximum comfort and support. Holland Bar Stool uses a detailed screen print process that applies specially formulated epoxy-vinyl ink in numerous stages to produce a sharp, crisp, clear image. You can't find a higher quality logo stool on the market. The plating grade steel used to build the frame is commercial...Seat Material: UpholsteredFrame Material: Metal
10 Jupiter Series 22 Bar Stool OFM
The furniture is almost always made of wood, and prior to the 19th century, unique to each home.
The patio rooms are efficient thermally due to 6" heavy duty aluminum framework encased with vinyl.
With its classic lines and restoration appeal, this counter height stool is the perfect way to seat guests at your dining table. This chair is made of solid hardwood in a rich gray finish that is a timeless blend with just the right amount of distressing. A solid back and padded seat are upholstered in beige fabric.Seat Material: UpholsteredFrame Material: Solid + Manufactured WoodUpholstery Material: FabricWeight Capacity: 200lb.Base Color: Grey/Gray
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Where to Find Bradberry Metal 24 Bar Stool (Set Of 2)
this valuable specific deal or promotion is 20-60% off. We would suggest Bradberry Metal 24 Bar Stool (Set Of 2). perfect price from the brand is special . confirmed customer satisfaction. Integrated! Price Bradberry Metal 24 Bar Stool (Set Of 2) starting from April 2019 with regard to you to get goods from a great many other stores, you are ready to update on Sunday-December-15-2019
04 Comments
Margarett Grisby2019-09-01
Love it. The Capri Blue is more of an light denim color rather than the teal I used to be expecting, but it's still very nice. It took me about 9 hours to put together alone with only hand tools. If you have a power screwdriver and a helper it will take significantly less time. I could've waited for my husband to truly have a day off to help but Personally i think pride in having built it without any help now! The product was very well packaged, all holes lined up perfectly, the parts were all obviously marked, and the directions (just diagrams, no written instructions) easy enough to check out. The seats are comfortable enough and the table is much larger plus more sturdy than I was expecting. I hope to take pleasure from my nook for quite some time to come! It dropped price your day after I got it, that is my only gripe! Bradberry Metal 24 Bar Stool (Set Of 2)
Marquis Schildgen2019-10-04
Great table. Super cute. Disappointed which it came in cracked. Would have given it 5 stars if no damage. Update: Just chatted with Mary S. from Wayfair Customer Service and they're sending replacement top! Wonder full customer service!!
Becki Damron2019-10-11
It took us a while to assemble the table and the chairs. No screw driver is a given the package allowing you to connect the table top using its base. Same applies to chairs cushion with the frame. The dining set fits well to your need. Overall, it looks durable and can handle rough consumption if you have children. I'd recommend it for those who are looking for economical but attractive dining set.
Dion Pekar2019-11-22
Proved great, but just retain in mind that it is definitely more of a cream color. The unit took about 3-4 hours for me personally to complete and I did so alone. Two people doing it together may possibly be better and a lot faster. I added handy remote control puck lights to the glass areas and it looks very pretty during the night. For those with kids, I was able to get safety 1st magnetic locks to work great on the doors and an anti-tip chain on the back. The drawers may be another story since there is nothing between your two drawers so there is no where to mount the catch for the latch. I just opted to keep the drawer contents kid friendly. I hadn't had a chance to mount the locks to the middle cabinet yet, but I'm pretty detain it will use the latch's on underneath corners of the doors and the catch's on the bottom shelf in the middle. The anti-tip chain mounted ok to the solid top. How strong it is, I'm uncertain but it appeared like solid wood. I'm not sure much weight will maintain the top of the unit so not sure it's a huge tip risk.


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Breast Cancer
Can Itchy/pain w/ no visible signs be IBC?
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Can Itchy/pain w/ no visible signs be IBC?
For 4 days now my left breast has been itchy from under my arm to surrounding my nipple. On saturday I noticed it was itchy but thought nothing of it. By sunday morning when I had been woken up a few times during the night and it was still there 24 hrs later I became concerned. There is nothing visibly wrong with the outside of my breast (no redness, change in skin texture, bumps, lumps). After it still being itchy yesterday morning and again getting woken up by itchiness through out the night I went to the doctors. She observed the same thing I did, nothing visible. However when she was palpating I did have some pain. I'm scheduled for an ultrasound on friday morning.
Unfortunately about 4 hours after I left the doctors, my breast started to hurt and itch at the same time. The closest description I could come up with is that it feels like a pimple does when it doesn't come to a head (itchy, sore, and pressure).
The first thing that came to my mind on sunday morning when it was just itching was IBC. Over a year ago I saw a news story about it. It was about a women who happend to get it while she was nursing, which my best friend was doing at the time, so it stuck out in my mind. I just remembered that one of the signs of it was itchiness. What concerns me is I know it is hard to diagnois to begin with, and it doesn't show up in ultrasounds, although ultrasound may show abnormalities in the lymph nodes. I'm basically wondering if my ultrasound comes back negative, should I go back to the doctor with my concerns?
As far as a little history, I'm 31. I do have some risk factors, I have large dense breasts, my grandmother and aunt did have tumors removed although they were benign, my great aunt did have breast cancer and had to get a masectomy, and I have been on depo-provera for 5 years.
I know I may be over reacting but everytime I do a search on itchiness I come back with a bunch of websites about breast cancer, which doesn't help. Although my symptoms can point towards a cyst, which are fairly common, and which I hope it is, I like to be well informed. Which is why I decided to post and see if there is a possibility that it could be IBC even though I'm not showing any physical signs.
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Wow, I just came across your post. I just posted a similar one a few minutes ago. I noticed no one had answered your question yet, but I wanted to at least let you know that you're not alone and I have the same questions myself. I have not made a doctor's appt yet. I hope you (and I) hear from someone soon...
Have you tried taking benadryl or putting neosporin cream on it. It sounds like an allergy.
I have not. The itching/pain isn't on the skin it is inside the breast. I don't think it is an allergy. I have allergies to many things, and this doesn't feel like that. I can only use certain soaps, certain shampoos/conditioners otherwise I get eczema. I can't wear makeup either, my eyes either itch like crazy, I get a rash, or I break out in zits. Also if I pet a cat and touch my face, my neck and face breakout in hives/red blotches. My breast skin is completely smooth (minus the stretch marks that I have always had), and white as white can be, there isn't any bumps either. The pain/itchiness pretty much takes up the whole left side of my breast. The itchiness is there constantly it goes from I can feel a pressure type itchiness to I HAVE TO SCRATCH NOW. The pain occurs when I move around or press against it. Although I found if press my left arm into the side it doesn't hurt as much when I walk.
A related discussion,
I have pain under my right breast
was started.
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This Esikhaweni house is in H2 section. It has 2 bedrooms, 1 bathroom, lounge, open plan kitchen, partial Aluminium windows, Burglar guards and is fenced.
Phone: 0827912955
Email: email@example.com
The flat is close to transport routes, it has 2 bedrooms with build-in cupboards, lounge, 1 bathroom, place for the washing machine, open plan kitchen, aircon in the lounge, 1 car port, security guard at the gate, electric fence around the complex too.
This house is a great buy! It has 4 bedrooms, 3 bathrooms (MES), aircons, 2 lounges, dining room, modern kitchen, patio, pool, 2 car ports, 1 garage, electric fence, alarm with loads of fruit trees to enjoy too.
This Starter Home has 3 bedrooms, 2 bathrooms (MES), lounge and dining room are open plan, kitchen and 1 Garage.
Farmland for rent at R1000 per hectare. It is around 7km from Empangeni.
There is up to 50 hectares available
These flats are walking distance from primary school & high school, from take away resturants, Walking distance from Spar and all transport also - Taxis route and bus route.
2 Bedrooms, 1 bathroom, open plan fitted kitchen, lounge, 1 car port, also good security with an Electric fence around the Complex. It includes water, you pay your own power!
The rent of R5300 applies for a 1 year contract with 1 month deposit. Renewals will be annual and will go up R400 per year.
If persons want 6 month contracts it R6000 per month and R6000 deposit. If persons want month to month leases it will be R7500 PER MONTH AND R7500 DEPOSIT
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Esikhaweni Rental - It is a modern Bachelor flat with open plan granite kitchen fitted with a stove,
Also 1 bathroom with shower, there are build-in cupboards.
This flat has 2 bedrooms, 1 bathroom, lounge, dining room and kitchen with 1 car port. It has been newly tiled out and renovated.


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Pink Pineapple Leggings - Turquoise and Pink Pineapples on dark navy blue Buttery soft leggings, with elastic waist
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Sotheby's International Realty - Escazú, SJ
Located in one of the most elegant and strategically located luxury compounds of the Central Valley, this unit is fantastic and priced to sell! At almost four thousand square feet of build, the apartment has three large bedrooms and service quarters, as well as a huge living room. The layout is such that there is natural light and ventilation on both the North side and the South side of the apartment, and it even has windows to the West, giving it three frontages. The North side has a covered terrace offering great views and large enough to host a party. The kitchen is very comfortable, with an oversize two-door fridge, plenty of counter and shelf space, and granite countertops. The master bathroom offers a view of the sunset to the West from the jacuzzi tub! Condominium amenities include a pool, pool house fully equipped, play areas, tennis courts, and gardens with mature full-grown trees offering shade and nice walks among the trees.
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Style: Casual
Fit Type: Loose
Collar-line: V Collar
Sleeves Length: Short Sleeves
Material: Cotton,Polyester
Waist Type: High
Closure Type: Zipper Fly
Front Style: Flat
Pattern Type: Floral
Season: Spring
Weight: 0.3900kg
Package: 1 x Top 1 x Pants
Tie Front Floral Print Top And Pants Set - Yellow M
Flash sale
Only left
Fit EU Size:38 Bust:36.22 Pants Waist:28.35 Hips:42.13 Pants Length:36.61 Top Length:14.57 Sleeve Length:15.35.(In inches)
sorry, this size was sold out.
is a size M
Height: 5'8"
Bust: 34"
Waist: 24"
Hip: 37"
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