Landscape




$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =





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.

#TheorySuperpotentialCentral charge $a$Central charge $c$Ratio $a/c$Matter field: $R$-chargeU(1) part of $F_{UV}$Rank of $F_{UV}$Rational
3029 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{3}M_{7}$ 0.6654 0.8297 0.8019 [M:[1.1705, 1.0814, 0.9631, 0.8295, 0.8295, 0.7558, 1.0369], q:[0.7704, 0.3556], qb:[0.4739, 0.563], phi:[0.4593]] [M:[[8], [-4], [10], [-8], [-8], [12], [-10]], q:[[-1], [3]], qb:[[-11], [1]], phi:[[2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{6}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{7}$, ${ }M_{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{5}q_{1}q_{2}$ ${}$ -2 t^2.267 + 2*t^2.488 + t^2.756 + t^3.111 + t^3.244 + t^3.378 + t^3.866 + t^4. + t^4.134 + t^4.221 + t^4.488 + t^4.535 + 3*t^4.756 + 3*t^4.977 + t^5.023 + 2*t^5.244 + 2*t^5.512 + 2*t^5.599 + t^5.733 + 3*t^5.866 - 2*t^6. + t^6.134 + t^6.221 + 2*t^6.355 + t^6.401 + 3*t^6.488 + t^6.622 + 2*t^6.71 + t^6.802 + 3*t^6.977 + 2*t^7.023 + 6*t^7.244 + t^7.29 + t^7.332 - t^7.378 + 4*t^7.465 + 3*t^7.512 + t^7.599 - t^7.645 + 2*t^7.733 + 2*t^7.779 + t^7.866 + 2*t^8. + 4*t^8.087 + t^8.134 + t^8.221 - t^8.267 + 5*t^8.355 + t^8.442 - 5*t^8.488 + 3*t^8.622 + t^8.668 + 3*t^8.71 - 2*t^8.756 + 2*t^8.843 + 2*t^8.889 + 6*t^8.977 - t^4.378/y - t^6.645/y - t^6.866/y + (2*t^7.756)/y + t^7.889/y + t^7.977/y + t^8.023/y + t^8.111/y + (2*t^8.244)/y + t^8.378/y + t^8.512/y + (2*t^8.599)/y + t^8.645/y + (2*t^8.733)/y + (3*t^8.866)/y - t^8.913/y - t^4.378*y - t^6.645*y - t^6.866*y + 2*t^7.756*y + t^7.889*y + t^7.977*y + t^8.023*y + t^8.111*y + 2*t^8.244*y + t^8.378*y + t^8.512*y + 2*t^8.599*y + t^8.645*y + 2*t^8.733*y + 3*t^8.866*y - t^8.913*y g1^12*t^2.267 + (2*t^2.488)/g1^8 + g1^4*t^2.756 + t^3.111/g1^10 + t^3.244/g1^4 + g1^2*t^3.378 + t^3.866/g1^6 + t^4. + g1^6*t^4.134 + t^4.221/g1^20 + t^4.488/g1^8 + g1^24*t^4.535 + 3*g1^4*t^4.756 + (3*t^4.977)/g1^16 + g1^16*t^5.023 + (2*t^5.244)/g1^4 + 2*g1^8*t^5.512 + (2*t^5.599)/g1^18 + t^5.733/g1^12 + (3*t^5.866)/g1^6 - 2*t^6. + g1^6*t^6.134 + t^6.221/g1^20 + (2*t^6.355)/g1^14 + g1^18*t^6.401 + (3*t^6.488)/g1^8 + t^6.622/g1^2 + (2*t^6.71)/g1^28 + g1^36*t^6.802 + (3*t^6.977)/g1^16 + 2*g1^16*t^7.023 + (6*t^7.244)/g1^4 + g1^28*t^7.29 + t^7.332/g1^30 - g1^2*t^7.378 + (4*t^7.465)/g1^24 + 3*g1^8*t^7.512 + t^7.599/g1^18 - g1^14*t^7.645 + (2*t^7.733)/g1^12 + 2*g1^20*t^7.779 + t^7.866/g1^6 + 2*t^8. + (4*t^8.087)/g1^26 + g1^6*t^8.134 + t^8.221/g1^20 - g1^12*t^8.267 + (5*t^8.355)/g1^14 + t^8.442/g1^40 - (5*t^8.488)/g1^8 + (3*t^8.622)/g1^2 + g1^30*t^8.668 + (3*t^8.71)/g1^28 - 2*g1^4*t^8.756 + (2*t^8.843)/g1^22 + 2*g1^10*t^8.889 + (6*t^8.977)/g1^16 - (g1^2*t^4.378)/y - (g1^14*t^6.645)/y - t^6.866/(g1^6*y) + (2*g1^4*t^7.756)/y + (g1^10*t^7.889)/y + t^7.977/(g1^16*y) + (g1^16*t^8.023)/y + t^8.111/(g1^10*y) + (2*t^8.244)/(g1^4*y) + (g1^2*t^8.378)/y + (g1^8*t^8.512)/y + (2*t^8.599)/(g1^18*y) + (g1^14*t^8.645)/y + (2*t^8.733)/(g1^12*y) + (3*t^8.866)/(g1^6*y) - (g1^26*t^8.913)/y - g1^2*t^4.378*y - g1^14*t^6.645*y - (t^6.866*y)/g1^6 + 2*g1^4*t^7.756*y + g1^10*t^7.889*y + (t^7.977*y)/g1^16 + g1^16*t^8.023*y + (t^8.111*y)/g1^10 + (2*t^8.244*y)/g1^4 + g1^2*t^8.378*y + g1^8*t^8.512*y + (2*t^8.599*y)/g1^18 + g1^14*t^8.645*y + (2*t^8.733*y)/g1^12 + (3*t^8.866*y)/g1^6 - g1^26*t^8.913*y


Deformation

Here is the data for the deformed fixed points from the chosen fixed point.

#SuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


Equivalent Fixed Points from Other Seed Theories

Here is a list of equivalent fixed points from other gauge theories.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore 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.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
1978 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ 0.6701 0.8368 0.8008 [M:[1.148, 1.0927, 0.9349, 0.852, 0.852, 0.7219], q:[0.7732, 0.3472], qb:[0.5049, 0.5602], phi:[0.4537]] t^2.166 + 2*t^2.556 + t^2.722 + t^2.805 + t^3.278 + t^3.361 + t^3.917 + t^4. + t^4.083 + t^4.332 + t^4.39 + t^4.556 + 3*t^4.722 + t^4.888 + t^4.971 + 3*t^5.112 + 2*t^5.278 + t^5.361 + 2*t^5.444 + t^5.527 + t^5.61 + t^5.834 + 2*t^5.917 - 2*t^6. - t^4.361/y - t^4.361*y detail