موضوع1:تازہ گوئی کا رجحان ( میر وسودا کا عہد)
میر تقی میر:
میر تقی میر اردو غزل کا نمائندہ شاعر ہے۔آج تک اس سطح کا کوئی شاعر ہمیں نہیں مل سکا۔ ان کی شاعری کے چھے دیوان چھپے۔ حال ہی میں ان کا ساتواں دیوان دریافت ہوا ہے۔ ڈاکٹر معین الدین عقیل صاحب نے مرتب کرکے یہ دیوان شائع کیا ہے۔
میر کا دور:
میر کا دور 1722ء سے 1810ء تک ہے اس میں کچھ اختلافات پائے جاتے ہیں۔ 1810ء میں ان کی وفات ہوئی میر کا زمانہ ایسا دور تھا جس میں ہر طرف بے چینی تھی۔دلی جو اس وقت مرکز تھا دارالحکومت تھا وہاں بہت سارے بیرونی حملہ آوروں نے بہت دفعہ حملہ کیا اس کی اینٹ سے اینٹ بجائی۔وہاں کے لوگ برباد ہو گئے ،قتل و غارت ہوئی ،خون بہا ،گھر اجڑ گئے ،اپنے بچھڑ گئے۔ان حالات کے اثرات اس وقت کے شعرا ء پر بہت گہرے پڑے۔ ان میں میر کا نام نمایاں ہے۔ میرکے والد کی وفات کے بعد ان کے چچا امان اللہ نے ان کی دیکھ بھال کی۔ ان کے چچا کی وفات کے بعد چچازاد بھائیوں نے گھر سے نکال دیا۔معاشی حالات بھی خراب تھے الغرض ایسے حالات میں میر بھٹکتے رہے۔مشکل حالات کا سامنا کرتے رہے۔ اس کے اثرات ان کی شاعری میں ہمیں نمایاں طور پر نظر آتے ہیں میر جیسا حساس شخص ان تکلیفوں میں مبتلا ہونے کے باوجود ان میں قنوطیت نظر نہیں آتی۔ ان کے دور میں مایوسی کا پہلو نظر نہیں آتا درد تو یقیناً ہے لیکن اس میں مایوسی نہیں۔ انہوں نے تہذیب کا بہت خوبصورتی سے مشاہدہ کیا اور اس کا عکس ان کی شاعری میں نظر آتا ہے۔ البتہ ان کی شاعری میں موت فنا کا ذکر زیادہ آتا ہے لیکن امید کی رمک ان کی شاعری میں جا بجا...
Islam always emphasizes to use legal ways and means of earning. In contrary the legal and illegal sources of income have been explained in detail. The “Right of invention” is one of the most discussed issues among the Islamic Jurists. This right is related to the intellectual skills and capabilities of people. However, internationally intellectual property is a known concept that associates with right of publication, right of trademark, patent and right of goodwill et cetera. However, research must be conducted on inquiring rights of intellectual property in Islamic Sharia and comparison of these rights with those in Western laws. In this paper the historical review of the intellectual properly has been presented. Similarly, those various types and concerned ruling have been discussed in contrast with the Islamic and western law on descriptive research methods.
Coherent Control of the Goos-Hänchen Shift The coherent control of the Goos-Hänchen (GH) shift has been investigated when a probe light is incident on a cavity which contains dispersive atomic medium. We consider different atom-field configurations for the intracavity atomic medium, i.e., electromagnetically induced transparency (EIT), Raman gain process and double L (duplicated two-level). The sub- and super-luminal pulse propagations which correspond to normal and anomalous dispersion, respectively, through a dispersive atomic medium can be coherently controlled without changing the structure. This is due to the manipulation of group index of the dispersive atomic medium via different parameters associated with the driving fields, i.e., intensity, detuning and phase shift. In this research thesis, we use these facts and report coherent control of the GH shift in the reflected and transmitted light when the light is incident on a cavity containing dispersive atomic medium. The positive and negative GH shifts in the reflected and transmitted light corresponding to the sub- and super-luminal propagation of the pulse, respectively, could be observed. We consider a cavity which is consisted of an intracavity medium and two dielectric slabs being the walls of the cavity. The thickness of each dielectric slab is d 1 and length of the intracavity medium is d 2 , i.e., the total length of the cavity is L = 2d 1 + d 2 . A TE-plane polarized probe light is incident on the cavity. We consider two types of intracavity media, i.e., three- and four-level EIT atomic configuration. Following the EIT configuration of the atom-field system inside the cavity, we observe a coherent control of the GH shifts via the intensity and detuning of the driving fields. We observe negative and positive GH shift in the reflected beam via intensity of the driving fields, however, only positive GH shift is observed in the transmitted light. This is due to the fact that the group index of the cavity which includes the dielectric slabs and intracavity medium becomes negative and positive for the corresponding negative and positive group index of the intracavity medium, respectively, however, it remains positive for the transmitted light. xTo reduce the strong absorption during super-luminal propagation of light, we suggest a gain-assisted model to control the GH shifts which is experimentally more viable scheme. In this scheme, a similar kind of control over sup- and sub- luminal light propagation can be achieved using three- and four-level atoms inside the cavity following one and two-photon Raman transitions. Both atomic systems exhibit gain-assisted super-luminal propagation of the light. First we consider three-level atomic system and observe a control over GH shift in the reflected and transmitted light via probe field detuning and intensity of the control field using three-level system. We observe negative GH shifts in the transmitted light and both positive and negative GH shift in the reflected light via manipulation of the optical susceptibility of the atomic medium. This is again due to the fact that the group index of the total cavity remains negative for the transmitted light whereas it could be positive and negative for the reflected light. Next, we consider four-level atomic system with N-type configuration and study the behavior of spatial as well as angular GH shifts for different choices of the control field. Finally, we consider a duplicated two-level atomic system, which is a degenerated double lambda system, inside the cavity and study the GH shift behavior corresponding to the super- and sub-luminal propagation of an incident Gaussian- shaped probe light. The system has a coherent control over the group velocity via the phase shift associated with the driving and probe fields and is independent of the intensity of the field in the low optical regime. We study influence of the width of the incident Gaussian probe light on GH shift and distortion. We observe a strong dependence of the GH shift and distortion of the pulse on the width of the incident light.