> On 4 Nov 2018, at 21:32, Jesse Mazer <laserma...@gmail.com> wrote: > > > > On Wed, Oct 31, 2018 at 7:30 AM Bruno Marchal <marc...@ulb.ac.be > <mailto:marc...@ulb.ac.be>> wrote: > >> On 30 Oct 2018, at 14:21, agrayson2...@gmail.com >> <mailto:agrayson2...@gmail.com> wrote: >> >> >> >> On Tuesday, October 30, 2018 at 8:58:30 AM UTC, Bruno Marchal wrote: >> >>> On 29 Oct 2018, at 13:55, agrays...@gmail.com <> wrote: >>> >>> >>> >>> On Monday, October 29, 2018 at 10:22:02 AM UTC, Bruno Marchal wrote: >>> >>>> On 28 Oct 2018, at 13:21, agrays...@gmail.com <> wrote: >>>> >>>> >>>> >>>> On Sunday, October 28, 2018 at 9:27:56 AM UTC, Bruno Marchal wrote: >>>> >>>>> On 25 Oct 2018, at 17:12, agrays...@gmail.com <> wrote: >>>>> >>>>> >>>>> >>>>> On Tuesday, October 23, 2018 at 10:39:11 PM UTC, agrays...@gmail.com >>>>> <http://gmail.com/> wrote: >>>>> If a system is in a superposition of states, whatever value measured, >>>>> will be repeated if the same system is repeatedly measured. But what >>>>> happens if the system is in a mixed state? TIA, AG >>>>> >>>>> If you think about it, whatever value you get on a single trial for a >>>>> mixed state, repeated on the same system, will result in the same value >>>>> measured repeatedly. If this is true, how does measurement distinguish >>>>> superposition of states, with mixed states? AG >>>> >>>> That is not correct. You can distinguish a mixture of particles in the up >>>> or down states with a set of 1/sqrt(2)(up+down) by measuring them with the >>>> {1/sqrt(2)(up+down), 1/sqrt(2)(up-down}) discriminating apparatus. With >>>> the mixture, half the particles will be defected in one direction, with >>>> the pure state, they will all pass in the same direction. Superposition >>>> would not have been discovered if that was not the case. >>>> >>>> And someone will supply the apparatus measuring (up + down), and (up - >>>> down)? No such apparatuses are possible since those states are inherently >>>> contradictory. We can only measure up / down. AG >>> >>> You can do the experience by yourself using a simple crystal of calcium >>> (CaCO3, Island Spath), or with polarising glass. Or with Stern-Gerlach >>> devices and electron spin. Just rotating (90° or 180°) an app/down >>> apparatus, gives you an (up + down)/(up - down) apparatus. >>> >>> I don't understand. With SG one can change the up/down axis by rotation, >>> but that doesn't result in an (up + down), or (up - down) measurement. If >>> that were the case, what is the operator for which those states are >>> eigenstates? Which book by Albert? AG >> >> David Z Albert, Quantum Mechanics and Experience, Harvard University Press, >> 1992. >> https://www.amazon.com/Quantum-Mechanics-Experience-David-Albert/dp/0674741137 >> >> <https://www.amazon.com/Quantum-Mechanics-Experience-David-Albert/dp/0674741137> >> >> Another very good books is >> >> D’Espagnat B. Conceptual foundations of Quantum mechanics, I see there is a >> new edition here: >> https://www.amazon.com/Conceptual-Foundations-Quantum-Mechanics-Advanced/dp/0738201049/ref=sr_1_1?s=books&ie=UTF8&qid=1540889778&sr=1-1&keywords=d%27espagnat+conceptual+foundation+of+quantum+mechanics&dpID=41NcluHD6fL&preST=_SY291_BO1,204,203,200_QL40_&dpSrc=srch >> >> <https://www.amazon.com/Conceptual-Foundations-Quantum-Mechanics-Advanced/dp/0738201049/ref=sr_1_1?s=books&ie=UTF8&qid=1540889778&sr=1-1&keywords=d%27espagnat+conceptual+foundation+of+quantum+mechanics&dpID=41NcluHD6fL&preST=_SY291_BO1,204,203,200_QL40_&dpSrc=srch> >> >> It explains very well the difference between mixtures and pure states. >> >> Bruno >> >> Thanks for the references. I think I have a reasonable decent understanding >> of mixed states. Say a system is in a mixed state of phi1 and phi2 with some >> probability for each. IIUC, a measurement will always result in an >> eigenstate of either phi1 or phi2 (with relative probabilities applying). > > If the measurement is done with a phi1/phi2 discriminating apparatus. Keep in > mind that any state can be seen as a superposition of other oblique or > orthogonal states. > > I don't know if you're restricting the definition of phi1 and phi2 to some > particular type of eigenstate or not, but in general aren't there pure states > that are not eigenstates of any physically possible measurement apparatus, so > there is no way to directly measure that a system is in such a state?

I limit myself to spin or polarisation. In some case there are selection or superselection rule, like with charge or other possible physical attribute, but not here. I use only the core formalism of quantum mechanics, where a change of base is a change of the experimental device, like a rotation of some Stern-Gerlach apparatus. Bruno > > -- > You received this message because you are subscribed to the Google Groups > "Everything List" group. > To unsubscribe from this group and stop receiving emails from it, send an > email to everything-list+unsubscr...@googlegroups.com > <mailto:everything-list+unsubscr...@googlegroups.com>. > To post to this group, send email to everything-list@googlegroups.com > <mailto:everything-list@googlegroups.com>. > Visit this group at https://groups.google.com/group/everything-list > <https://groups.google.com/group/everything-list>. > For more options, visit https://groups.google.com/d/optout > <https://groups.google.com/d/optout>. -- You received this message because you are subscribed to the Google Groups "Everything List" group. To unsubscribe from this group and stop receiving emails from it, send an email to everything-list+unsubscr...@googlegroups.com. To post to this group, send email to everything-list@googlegroups.com. Visit this group at https://groups.google.com/group/everything-list. For more options, visit https://groups.google.com/d/optout.