title: Ko ngā whakahokinga kōrero a te hunga uiui i roto i te akomanga rumaki i te Whare Wānanga o Waikato: He pūrongo mō ngā ui pātai

authors: Nock, Sophie

subjects: Reo Māori

abstract: Ko te whāinga matua o tēnei rangahau he whakakaokao, he wetewete āno hoki i ngā whakahokinga kōrero a te hunga uiui i kake atu ai ki runga i te waka o Te Tohu Paetahi i te tau 2008, i raro i te kōawa o Rehutai, i raro anō hoki i te maru o Te Whare Wānanga o Waikato. Ka aro atu ki ngā urupare a te hunga tekau mā ono mō te kaupapa nei o Te Tohu Paetahi, ka mutu, ka matapakihia ngā kōrero me ngā whakaaro o taua hunga kia āta kitea ai, āe rānei e tika ana te whakahaere, te mahi whakaako i te reo, te tautoko mai hoki a ngā kaiwhakaako me te kura. I te mutunga iho tautoko katoa te hunga uiui ki aua mea katoa.

text: Ko ngā whakahokinga kōrero a te hunga uiui i roto i te akomanga rumaki i te Whare Wānanga o Waikato: He pūrongo mō ngā ui pātai Ko te whāinga matua o tēnei rangahau he whakakaokao, he wetewete āno hoki i ngā whakahokinga kōrero a te hunga uiui i kake atu ai ki runga i te waka o Te Tohu Paetahi i te tau 2008, i raro i te kōawa o Rehutai, i raro anō hoki i te maru o Te Whare Wānanga o Waikato. Ka aro atu ki ngā urupare a te hunga tekau mā ono mō te kaupapa nei o Te Tohu Paetahi, ka mutu, ka matapakihia ngā kōrero me ngā whakaaro o taua hunga kia āta kitea ai, āe rānei e tika ana te whakahaere, te mahi whakaako i te reo, te tautoko mai hoki a ngā kaiwhakaako me te kura. I te mutunga iho tautoko katoa te hunga uiui ki aua mea katoa.

year: 2017

title: He hekenga toto, he hekenga tōtā, he hekenga roimata.

authors: Mikaere, Te Maharanui Jacob

abstract: Ariā
Ko tā te tuhinga nei he whakakite i ngā āwangawanga o te kaituhi mō te maha o te hunga taiohi kua tipu mai i raro i te ātaarangi o te Kōhanga Reo, o te Kura Kaupapa Māori, o te wharekura hoki, kua noho ko te reo Māori hei reo tuatahi, engari mō te aronui ki te reo me tōna katoa kore kore rawa atu. Kei te kōrerohia ōna hītori me tōna whakapapa. I ahu mai tō tāua reo i hea? I pēhea tō tāua reo i ngā wā o mua? I pēhea tō tāua reo i te taetanga mai o tauiwi i te takiwā o te 1800? I ahatia tō tāua reo e tauiwi i tērā rautau i kīa ake he reo koretake noa te reo Māori? Nā wai tō tāua reo i ruke ki rāhaki i ngā tau 1900? Ka mutu, nā wai tō tāua reo i whakahoki mai ki te kōpū o tēnei whakatipuranga? Nā ēnei tūmomo urupounamu au i karanga ki te ihi o tōku whare kōrero. 
Ko te ngako o ngā kōrero o roto i te tuhinga nei he whakatewhatewha, he matapaki i te kūare o te hunga taiohi ki te whakapapa, ki te hītori o te reo Māori. Koia ko ōna piki me ōna heke, ngā whakapātaritari i ngana ki te whakapoko i te ahi o te reo Māori i te tata whāngaromanga ōna. Ko te nuinga o ngā kōrero he mea rangahau mai i ngā pukapuka me te whakatakoto i ngā kitenga hei pānuitanga mā te hunga e tāpara ana ki ngā kai o roto. Me whakanui ka tika ngā pēhitanga o te hunga i takatakahi i te ara papatoiake hei whaitanga mā tātau ka tahi, ka rua me kōkuhu ēnei tūmomo mātauranga ki ngā marau whakaako tamariki me kore noa e tahuri mai te hunga taiohi ki tōna reo me tōna katoa. E ora ai te whakapapa o te reo me ōna hītori me whakakōpā e tātau  tōna whakapapa, me ōna kōrero ki ngā tamariki kōhanga mai, kura kaupapa mai, wharekura mai, ā huri atu ki ngā pia whare wānanga hoki. Mā te whakaako i te hītori ki a ngāi taiohi ākene pea ka tipu te kauanuanu ki tōna reo. Kia kekeno atu au ki tōku reanga kei te kitea he momo whakahīhī kua puea ake ai ki roto tonu i a tātau. Ko te momo o tēnei whakahīhī he mea tūkino i te hunga kore reo, he mea whakaiti i ngā tāngata kua noho rehurehu ki ngā kawenga a tāua te Māori. E whakapono ana au mā te kauanuanu o tōku reanga ki tōna reo ka tipu hoki te kauanuanu ki te hunga kāore pea i rongo i ngā hua o te reo, rātau te hunga kua noho pōhara, kua noho manene nā ngā rā pōkākā o te whakapākehātanga. Atu i te whakahīhī o te ngākau kua puea hoki tētahi momo e patu nei i te kōrerotanga o tō tātau reo, arā ake ko te ngākau māngere. I te korenga o te aronui o tōku reanga ki te reo kua tipu ake ētahi, ahakoa i pakeke mai i roto i te Kōhanga Reo mō te kōrero Māori atu kia pakeke ana rātau he aha te aha. Mā te ako i ngā hītori o tō tātau reo e titi ai ki te whatu manawa te hiranga o tō tātau reo, mā tērā e kore rawa te tangata e noho hāneanea me te pōhēhē ka pai noa te reo Māori, ka mutu kāore he tino take kia kaha kōrerotia. 
Ko te tino whāinga o tēnei tuhinga he ngana ki te whakarārangi mai ko hea te huarahi e tuwhera ai ngā kuaha o te ao Māori ki te katoa e tū rangatira ai tātau. Ahakoa pakeke mai taiohi mai rānei, ahakoa matatau ki te reo tauhou ki te reo rānei ko te mea nui kia tū whakahīhī, kia tū māia te iwi Māori ki raurangi.

text: He hekenga toto, he hekenga tōtā, he hekenga roimata. Ariā
Ko tā te tuhinga nei he whakakite i ngā āwangawanga o te kaituhi mō te maha o te hunga taiohi kua tipu mai i raro i te ātaarangi o te Kōhanga Reo, o te Kura Kaupapa Māori, o te wharekura hoki, kua noho ko te reo Māori hei reo tuatahi, engari mō te aronui ki te reo me tōna katoa kore kore rawa atu. Kei te kōrerohia ōna hītori me tōna whakapapa. I ahu mai tō tāua reo i hea? I pēhea tō tāua reo i ngā wā o mua? I pēhea tō tāua reo i te taetanga mai o tauiwi i te takiwā o te 1800? I ahatia tō tāua reo e tauiwi i tērā rautau i kīa ake he reo koretake noa te reo Māori? Nā wai tō tāua reo i ruke ki rāhaki i ngā tau 1900? Ka mutu, nā wai tō tāua reo i whakahoki mai ki te kōpū o tēnei whakatipuranga? Nā ēnei tūmomo urupounamu au i karanga ki te ihi o tōku whare kōrero. 
Ko te ngako o ngā kōrero o roto i te tuhinga nei he whakatewhatewha, he matapaki i te kūare o te hunga taiohi ki te whakapapa, ki te hītori o te reo Māori. Koia ko ōna piki me ōna heke, ngā whakapātaritari i ngana ki te whakapoko i te ahi o te reo Māori i te tata whāngaromanga ōna. Ko te nuinga o ngā kōrero he mea rangahau mai i ngā pukapuka me te whakatakoto i ngā kitenga hei pānuitanga mā te hunga e tāpara ana ki ngā kai o roto. Me whakanui ka tika ngā pēhitanga o te hunga i takatakahi i te ara papatoiake hei whaitanga mā tātau ka tahi, ka rua me kōkuhu ēnei tūmomo mātauranga ki ngā marau whakaako tamariki me kore noa e tahuri mai te hunga taiohi ki tōna reo me tōna katoa. E ora ai te whakapapa o te reo me ōna hītori me whakakōpā e tātau  tōna whakapapa, me ōna kōrero ki ngā tamariki kōhanga mai, kura kaupapa mai, wharekura mai, ā huri atu ki ngā pia whare wānanga hoki. Mā te whakaako i te hītori ki a ngāi taiohi ākene pea ka tipu te kauanuanu ki tōna reo. Kia kekeno atu au ki tōku reanga kei te kitea he momo whakahīhī kua puea ake ai ki roto tonu i a tātau. Ko te momo o tēnei whakahīhī he mea tūkino i te hunga kore reo, he mea whakaiti i ngā tāngata kua noho rehurehu ki ngā kawenga a tāua te Māori. E whakapono ana au mā te kauanuanu o tōku reanga ki tōna reo ka tipu hoki te kauanuanu ki te hunga kāore pea i rongo i ngā hua o te reo, rātau te hunga kua noho pōhara, kua noho manene nā ngā rā pōkākā o te whakapākehātanga. Atu i te whakahīhī o te ngākau kua puea hoki tētahi momo e patu nei i te kōrerotanga o tō tātau reo, arā ake ko te ngākau māngere. I te korenga o te aronui o tōku reanga ki te reo kua tipu ake ētahi, ahakoa i pakeke mai i roto i te Kōhanga Reo mō te kōrero Māori atu kia pakeke ana rātau he aha te aha. Mā te ako i ngā hītori o tō tātau reo e titi ai ki te whatu manawa te hiranga o tō tātau reo, mā tērā e kore rawa te tangata e noho hāneanea me te pōhēhē ka pai noa te reo Māori, ka mutu kāore he tino take kia kaha kōrerotia. 
Ko te tino whāinga o tēnei tuhinga he ngana ki te whakarārangi mai ko hea te huarahi e tuwhera ai ngā kuaha o te ao Māori ki te katoa e tū rangatira ai tātau. Ahakoa pakeke mai taiohi mai rānei, ahakoa matatau ki te reo tauhou ki te reo rānei ko te mea nui kia tū whakahīhī, kia tū māia te iwi Māori ki raurangi.

year: 2016

title: Nonequilibrium transitions in quantum optical systems

authors: Drummond, Peter David

abstract: The topic of this thesis is a theoretical study of nonequilibrium transitions and quantum statistical properties of nonlinear quantum optical systems driven by an external radiation source. In certain limiting cases, a comparison is made between these transitions and the phase transitions found in equilibrium physical systems.
In chapters one and two, the mathematical tools are introduced. In operator terms, the time development is described by a Markovian master equation in the interaction picture. This is equivalent to a corresponding time development equation or Fokker-Planck equation in a vector space of c-numbers. In order to deal with the type of Fokker-Planck equation that results, we introduce a quantum classical correspondence resulting in a distribution function over a complex phase-space, which is a generalisation of the Glauber-Sudarshan P-function.
In chapter three this is applied to a model of a coherently driven mode with nonlinear dispersion and absorption. We find in the limit of zero temperature, that the spectrum is symmetric relative to the input frequency, and an exact solution is obtained for the distribution function. For a detuned driving field and nonlinear dispersion, optical bistability can occur. 
In chapter four a model of sub/second harmonic generation is introduced. This has several non-equilibrium transitions, including dispersive optical bistability, and bistable behaviour with coherent phase-locked input to both modes. Exact solutions occur in the limit of zero temperature and adiabatic elimination of one mode. In both chapters three and four, steady-state photon anti-bunching occurs with an absorptive nonlinearity. 
In chapter five we include interactions between the radiation mode and a fluorescent atomic system. In this case different behaviour occurs depending on the relative decay rates of the individual atoms and of the radiation mode. In the case of a high-Q interferometer, the atomic variables can be adiabatically eliminated. Both dispersive and absorptive bistability can occur. We show by analytic and numerical calculations (in the case of inhomogeneous broadening) that dispersive operation has advantages in requiring a lower atomic density and input field to observe bistability. When the input field has Gaussian (rather than coherent) photon statistics, there is no bistability, but enhanced photon bunching occurs. 
Finally, there is a different type of behaviour when the field mode decays rapidly and can be adiabatically eliminated. Within the cooperation lifetime the system can be described by a J²-invariant Hamiltonian, giving the special case of only collective damping. The result is a new type of critical point transition in the thermodynamic limit, with the appearance of a family of solutions like Lotka-Volterra cycles for a coherent driving field above threshold.

text: Nonequilibrium transitions in quantum optical systems The topic of this thesis is a theoretical study of nonequilibrium transitions and quantum statistical properties of nonlinear quantum optical systems driven by an external radiation source. In certain limiting cases, a comparison is made between these transitions and the phase transitions found in equilibrium physical systems.
In chapters one and two, the mathematical tools are introduced. In operator terms, the time development is described by a Markovian master equation in the interaction picture. This is equivalent to a corresponding time development equation or Fokker-Planck equation in a vector space of c-numbers. In order to deal with the type of Fokker-Planck equation that results, we introduce a quantum classical correspondence resulting in a distribution function over a complex phase-space, which is a generalisation of the Glauber-Sudarshan P-function.
In chapter three this is applied to a model of a coherently driven mode with nonlinear dispersion and absorption. We find in the limit of zero temperature, that the spectrum is symmetric relative to the input frequency, and an exact solution is obtained for the distribution function. For a detuned driving field and nonlinear dispersion, optical bistability can occur. 
In chapter four a model of sub/second harmonic generation is introduced. This has several non-equilibrium transitions, including dispersive optical bistability, and bistable behaviour with coherent phase-locked input to both modes. Exact solutions occur in the limit of zero temperature and adiabatic elimination of one mode. In both chapters three and four, steady-state photon anti-bunching occurs with an absorptive nonlinearity. 
In chapter five we include interactions between the radiation mode and a fluorescent atomic system. In this case different behaviour occurs depending on the relative decay rates of the individual atoms and of the radiation mode. In the case of a high-Q interferometer, the atomic variables can be adiabatically eliminated. Both dispersive and absorptive bistability can occur. We show by analytic and numerical calculations (in the case of inhomogeneous broadening) that dispersive operation has advantages in requiring a lower atomic density and input field to observe bistability. When the input field has Gaussian (rather than coherent) photon statistics, there is no bistability, but enhanced photon bunching occurs. 
Finally, there is a different type of behaviour when the field mode decays rapidly and can be adiabatically eliminated. Within the cooperation lifetime the system can be described by a J²-invariant Hamiltonian, giving the special case of only collective damping. The result is a new type of critical point transition in the thermodynamic limit, with the appearance of a family of solutions like Lotka-Volterra cycles for a coherent driving field above threshold.

year: 1979