Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 57600 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}^{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{4}M_{7}$ | 0.6549 | 0.808 | 0.8105 | [M:[1.1744, 1.0, 0.8256, 0.7985, 1.1008, 0.6977, 1.2015], q:[0.3992, 0.4263], qb:[0.6008, 0.7752], phi:[0.4496]] | [M:[[-3], [0], [3], [-8], [4], [-12], [8]], q:[[-4], [7]], qb:[[4], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{3}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{5}$, ${ }M_{1}$, ${ }M_{7}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{6}$, ${ }M_{3}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{3}M_{5}$, ${ }M_{6}\phi_{1}q_{1}^{2}$ | ${}$ | -1 | t^2.093 + t^2.477 + t^3. + t^3.081 + t^3.302 + t^3.523 + t^3.605 + t^3.744 + t^3.826 + t^4.128 + t^4.186 + t^4.349 + t^4.43 + t^4.57 + 2*t^4.953 + t^5.093 + t^5.174 + t^5.558 + t^5.616 + t^5.698 + t^5.779 + t^5.837 - t^6. + t^6.081 + t^6.163 + t^6.221 + t^6.279 + t^6.302 + t^6.384 + t^6.442 + 2*t^6.605 + t^6.663 + t^6.686 + t^6.826 + 2*t^6.907 + 2*t^7.047 + t^7.128 + t^7.186 + t^7.209 + t^7.267 + 3*t^7.43 + t^7.488 + t^7.512 + t^7.57 + 2*t^7.651 + t^7.709 + t^7.733 + t^7.791 + t^7.93 + t^7.953 + 2*t^8.035 + t^8.174 + 2*t^8.256 + t^8.314 + t^8.372 - t^8.477 + t^8.535 + t^8.558 + t^8.639 + 2*t^8.698 + t^8.756 + t^8.779 + t^8.86 - t^4.349/y - t^6.442/y + t^7.57/y + t^8.093/y + t^8.174/y + t^8.256/y + t^8.395/y + t^8.477/y - t^8.535/y + t^8.558/y + t^8.616/y + t^8.698/y + t^8.779/y + t^8.837/y + t^8.919/y - t^4.349*y - t^6.442*y + t^7.57*y + t^8.093*y + t^8.174*y + t^8.256*y + t^8.395*y + t^8.477*y - t^8.535*y + t^8.558*y + t^8.616*y + t^8.698*y + t^8.779*y + t^8.837*y + t^8.919*y | t^2.093/g1^12 + g1^3*t^2.477 + t^3. + g1^11*t^3.081 + g1^4*t^3.302 + t^3.523/g1^3 + g1^8*t^3.605 + t^3.744/g1^10 + g1*t^3.826 + g1^5*t^4.128 + t^4.186/g1^24 + t^4.349/g1^2 + g1^9*t^4.43 + t^4.57/g1^9 + 2*g1^6*t^4.953 + t^5.093/g1^12 + t^5.174/g1 + g1^14*t^5.558 + t^5.616/g1^15 + t^5.698/g1^4 + g1^7*t^5.779 + t^5.837/g1^22 - t^6. + g1^11*t^6.081 + g1^22*t^6.163 + t^6.221/g1^7 + t^6.279/g1^36 + g1^4*t^6.302 + g1^15*t^6.384 + t^6.442/g1^14 + 2*g1^8*t^6.605 + t^6.663/g1^21 + g1^19*t^6.686 + g1*t^6.826 + 2*g1^12*t^6.907 + (2*t^7.047)/g1^6 + g1^5*t^7.128 + t^7.186/g1^24 + g1^16*t^7.209 + t^7.267/g1^13 + 3*g1^9*t^7.43 + t^7.488/g1^20 + g1^20*t^7.512 + t^7.57/g1^9 + 2*g1^2*t^7.651 + t^7.709/g1^27 + g1^13*t^7.733 + t^7.791/g1^16 + t^7.93/g1^34 + g1^6*t^7.953 + 2*g1^17*t^8.035 + t^8.174/g1 + 2*g1^10*t^8.256 + t^8.314/g1^19 + t^8.372/g1^48 - g1^3*t^8.477 + t^8.535/g1^26 + g1^14*t^8.558 + g1^25*t^8.639 + (2*t^8.698)/g1^4 + t^8.756/g1^33 + g1^7*t^8.779 + g1^18*t^8.86 - t^4.349/(g1^2*y) - t^6.442/(g1^14*y) + t^7.57/(g1^9*y) + t^8.093/(g1^12*y) + t^8.174/(g1*y) + (g1^10*t^8.256)/y + t^8.395/(g1^8*y) + (g1^3*t^8.477)/y - t^8.535/(g1^26*y) + (g1^14*t^8.558)/y + t^8.616/(g1^15*y) + t^8.698/(g1^4*y) + (g1^7*t^8.779)/y + t^8.837/(g1^22*y) + t^8.919/(g1^11*y) - (t^4.349*y)/g1^2 - (t^6.442*y)/g1^14 + (t^7.57*y)/g1^9 + (t^8.093*y)/g1^12 + (t^8.174*y)/g1 + g1^10*t^8.256*y + (t^8.395*y)/g1^8 + g1^3*t^8.477*y - (t^8.535*y)/g1^26 + g1^14*t^8.558*y + (t^8.616*y)/g1^15 + (t^8.698*y)/g1^4 + g1^7*t^8.779*y + (t^8.837*y)/g1^22 + (t^8.919*y)/g1^11 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
| id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
|---|
Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 55908 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}^{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ | 0.6719 | 0.8383 | 0.8015 | [M:[1.1688, 1.0, 0.8312, 0.7836, 1.1082, 0.6754], q:[0.3918, 0.4394], qb:[0.6082, 0.7771], phi:[0.4459]] | t^2.026 + t^2.351 + t^2.493 + t^3. + t^3.143 + t^3.325 + t^3.507 + t^3.688 + t^3.831 + t^4.052 + t^4.156 + t^4.338 + t^4.377 + t^4.48 + t^4.52 + t^4.701 + t^4.844 + 2*t^4.987 + t^5.026 + t^5.169 + t^5.351 + t^5.493 + t^5.533 + t^5.636 + t^5.675 + t^5.714 + t^5.818 + t^5.857 - t^6. - t^4.338/y - t^4.338*y | detail |