Bitter decoration and magneto-optical studies reveal that in heavy-ion irradiated superconductors, a 'porous' vortex matter is formed when vortices outnumber columnar defects (CDs). In this state ordered vortex crystallites are embedded in the 'pores' of a rigid matrix of vortices pinned on CDs. The crystallites melt through a first-order transition while the matrix remains solid. The melting temperature increases with density of CDs and eventually turns into a continuous transition. At high temperatures a sharp kink in the melting line is found, signaling an abrupt change from crystallite melting to melting of the rigid matrix.PACS numbers: 74.60. Ec, 74.60.Ge, 74.72.Hs Melting of heterogeneous systems, and in particular of nanocrystals embedded in porous rigid matrices, is a complex process with many uncontrolled parameters. Metal and semiconductor nanocrystals with free surfaces, for example, usually show a decrease in their melting temperature with decreasing size [1], whereas nanocrystals encapsulated in a porous matrix often display an increase in melting temperature [2]. Although the contribution of the different factors is still a matter of debate, the melting process is known to depend on the size, dimensionality, material properties of the nanocrystals and the matrix, as well as the interface energies between the materials [1,2]. In this work we investigate an analogous, but a more controllable composite system, which is a 'porous' vortex matter consisting of vortex nanocrystals encapsulated in a matrix of strongly pinned vortices. As shown below, this system is present in the commonly heavy-ion irradiated superconductors when the vortices outnumber the columnar defects (CDs). The rigid matrix is created by vortices localized on the network of random CDs, while the softer nanocrystals are formed within the 'pores' of this matrix by the interstitial vortices. The size of the nanocrystals can be readily varied from several hundred down to a few vortices by changing the applied field or the density of CDs. We find that this composite vortex matter reveals a number of intriguing mechanisms: Similarly to the metallic nanocrystals in a matrix, we observe for the first time a pronounced upward shift in the vortex melting temperature T m , while preserving the first-order nature of the transition (FOT). With increasing density of CDs, the size of the pores decreases, resulting in a larger shift in T m . We also find a critical point at which the FOT changes into a continuous melting. Moreover, the crystallites can melt while the matrix remains rigid. As a result, at high temperatures we find an abrupt breakdown in the upward shift of T m and a sharp kink in the FOT line, which apparently result from the collapse of the matrix due to vortex depinning from the CDs.The reported findings were obtained using Bitter decoration and differential magneto-optical (MO) [3] techniques. High quality Bi 2 Sr 2 CaCu 2 O 8 (BSCCO) crystals (T c ≈ 89 K) were covered by various patterned masks and irradiated at GANIL by 1 Ge...
Magnetic screening response of the superconductor 2H-NbSe 2 with varying pinning reveals a rich evolution of the peak effect from a history-independent sharp anomaly to a broad and strongly history dependent effect with internal structure. The results display a stepwise disordering of the vortex lattice through transformations affected by both thermal fluctuations and quenched disorder. ͓S0163-1829͑99͒03309-3͔ PHYSICAL REVIEW B
A study of path dependent effects in single crystals of CeRu2 and 2H − N bSe2 show that critical current density Jc of the vortex state depends on its thermomagnetic history over a very large part of (H, T ) parameter space. The path dependence in Jc is absent above the peak position (i.e., H > Hp) of the peak effect region, which we believe identifies the complete loss of order in the vortex structure. The highly disordered FC state can be healed into a relatively ordered vortex lattice by subjecting it to a large enough change in dc field (few tens of Oe) or by shaking the FC state with sufficient ac field (few Oe).
Using a differential magneto-optical technique to visualize flow of transport currents, we reveal a new delocalization line within the reversible vortex liquid region in the presence of a low density of columnar defects. This line separates a homogeneous vortex liquid, in which all the vortices are delocalized, from a heterogeneous "nanoliquid" phase, in which interconnected nanodroplets of vortex liquid are caged in the pores of a solid skeleton formed by vortices pinned on columnar defects. The nanoliquid phase displays high correlation along the columnar defects but no transverse critical current.PACS numbers: 74.25. Qt, 74.25.Op, 74.25.Sv, 74.72.Hs Columnar defects (CDs) created in high-temperature superconductors by high-energy heavy ion irradiation act as very efficient pinning centers for vortices aligned along the CDs. The effects of this correlated disorder on the vortex properties have been investigated extensively mainly in the limit of relatively high density of CDs where the enhancement in the critical current for practical applications is most significant and the vortex matter is known to form the Bose glass phase [1][2][3][4]. In contrast, our understanding of the opposite limit, in which sparse CDs perturb a higher concentration of vortices, is still incomplete. Recent experimental studies [5,6] have shown that in this case the vortex matter can no longer be regarded as a homogeneously pinned medium. Instead, an intrinsically heterogeneous structure with two distinct sub-systems of vortices with very different characteristic energies is formed: vortices residing on CDs are strongly pinned and create a rigid skeleton, while the interstitial vortices form relatively ordered nanocrystals intercalated within the voids of this porous skeleton. This experimental finding of a "porous" vortex solid has contributed to a series of recent theoretical studies and numerical simulations [7][8][9][10][11][12]. Moreover, it was found that the melting line B m (T ) of the "porous" vortex solid has an unconventional behavior showing a pronounced kink [5,6]. This has led to the suggestion of the possible existence of two different liquid phases: at fields below the kink a usual homogeneous vortex liquid is formed upon melting, whereas at fields above the kink the "porous" solid melts into a heterogeneous state in which liquid vortices coexist with a skeleton of pinned vortices. It was proposed that in such a case a new transition line separating these two liquid phases should be expected [5,3,10]. Using a new imaging technique we present here the first experimental evidence for such a transition line within the reversible vortex liquid phase that separates a heterogeneous "nanoliquid" from a homogeneous liquid. One of the interesting properties of this novel nanoliquid phase is the absence of in-plane dissipationless superconductivity, while the coherence along the c-axis is apparently still preserved. The CDs were created along the c-axis in Bi 2 Sr 2 CaCu 2 O 8 (BSCCO) single crystals (T c ≃ 90 K) using low ir...
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